CHMO, the chemical methods ontology, describes methods used to collect data in chemical experiments, such as mass spectrometry and electron microscopy prepare and separate material for further analysis, such as sample ionisation, chromatography, and electrophoresis synthesise materials, such as epitaxy and continuous vapour deposition It also describes the instruments used in these experiments, such as mass spectrometers and chromatography columns. It is intended to be complementary to the Ontology for Biomedical Investigations (OBI).
Chemical Methods Ontology
1.2
batchelorc
definition
Non-mining synonym
synonym_type_property
has_alternative_id
database_cross_reference
has_exact_synonym
has_narrow_synonym
has_obo_format_version
has_related_synonym
has_scope
has_synonym_type
in_subset
BFO:0000052
inheres_in
BFO:0000054
realized in
BFO:0000056
participates in at some time
BFO:0000057
has participant
BFO:0000068
begins to exist during
BFO:0000069
ceases to exist during
BFO:0000085
has function at some time
BFO:0000087
has role
BFO:0000110
has continuant part at all times
BFO:0000118
has proper occurrent part
BFO:0000137
proper part of continuant at all times
BFO:0000174
has proper continuant part at some time
BFO:0000175
proper part of continuant at some time
BFO:0000178
has continuant part at some time
CHMO:0002748
p has_participant e o e has_role analyte_role. Don't know how to do this in OBO format.
has analyte
CHMO:0002883
p has_participant e o e has_role matrix_role. Don't know how to do this in OBO format.
has matrix
A process p probes_atom n if it has_participant n and its objective o is to determine the energy levels of n.
CHMO:0002922
should really be probes_nucleus but ChEBI doesn't have the nuclei. Will use atoms for now.
probes_atom
A process p probes_atom n if it has_participant n and its objective o is to determine the energy levels of n.
https://orcid.org/0000-0001-5985-7429
CHMO:0010016
the range of 'prevents' is an adverse laboratory event (process). The object that prevents the ALE blocks a disposition that is manifested as the ALE. Example: water blocks flammability. From a safety officer pov, this is about planning.
prevents
CHMO:0010017
the range of 'mitigates' is an adverse laboratory event (process). The object that mitigates the ALE has the capability (disposition) to take part in the process and prevent downstream adverse events. From a safety officer pov, this is about responding.
mitigates
IAO:0000136
is_about
OBI:0000293
has_specified_input
OBI:0000299
has_specified_output
OBI:0000312
is_specified_output_of
This relation obtains between a planned process and a objective specification when the criteria specified in the objective specification are met at the end of the planned process.
OBI:0000417
achieves_planned_objective
This relation obtains between a planned process and a objective specification when the criteria specified in the objective specification are met at the end of the planned process.
obi:ar
obi:bp
p is causally upstream of q if and only if p precedes q and p and q are linked in a causal chain
Chris Mungall
RO:0002411
causally upstream of
BFO:0000002
continuant
ic
IndependentContinuant
a chair
a heart
a leg
a molecule
a spatial region
an atom
an orchestra.
an organism
the bottom right portion of a human torso
the interior of your mouth
b is an independent continuant = Def. b is a continuant which is such that there is no c and no t such that b s-depends_on c at t. (axiom label in BFO2 Reference: [017-002])
http://purl.obolibrary.org/obo/bfo/2019-08-26/bfo.owl
For any independent continuant b and any time t there is some spatial region r such that b is located_in r at t. (axiom label in BFO2 Reference: [134-001])
For every independent continuant b and time t during the region of time spanned by its life, there are entities which s-depends_on b during t. (axiom label in BFO2 Reference: [018-002])
(forall (x t) (if (IndependentContinuant x) (exists (r) (and (SpatialRegion r) (locatedInAt x r t))))) // axiom label in BFO2 CLIF: [134-001]
(forall (x t) (if (and (IndependentContinuant x) (existsAt x t)) (exists (y) (and (Entity y) (specificallyDependsOnAt y x t))))) // axiom label in BFO2 CLIF: [018-002]
(iff (IndependentContinuant a) (and (Continuant a) (not (exists (b t) (specificallyDependsOnAt a b t))))) // axiom label in BFO2 CLIF: [017-002]
BFO:0000004
independent continuant
BFO:0000015
process
BFO:0000016
disposition
BFO:0000017
realizable_entity
BFO:0000019
quality
BFO:0000020
specifically dependent continuant
BFO:0000023
role
BFO:0000031
generically dependent continuant
BFO:0000034
function
BFO:0000040
material entity
BFO:0000140
continuant fiat boundary
Any constitutionally or isotopically distinct atom, molecule, ion, ion pair, radical, radical ion, complex, conformer etc., identifiable as a separately distinguishable entity.
CHEBI:23367
molecular entity
CHEBI:23377
copper molecular entity
CHEBI:28262
dimethyl sulfoxide
CHEBI:28694
copper atom
CHEBI:33418
graphite
CHEBI:33819
oxygen-17 atom
CHEBI:35255
chloroform
CHEBI:36928
carbon-13 atom
CHEBI:36940
fluorine-19 atom
CHEBI:46729
vitreous silica
CHEBI:50594
carbon nanotube
CHEBI:50795
nanostructure
CHEBI:50796
nanotube
CHEBI:50803
nanoparticle
CHEBI:50825
gold nanoparticle
CHEBI:52230
tin-119 atom
CHEBI:52455
lead-207
CHEBI:52456
vanadium-51 atom
CHEBI:52458
lithium-7 atom
CHEBI:52462
tungsten-183
CHEBI:60004
mixture
CHEBI:60027
polymer
true
The determination of the spectral absorbance of a solution. This method is often used to determine the concentration of a chemical in a solution.
colorimetric method
colourimetry
CHMO:0000001
colorimetry
The determination of the spectral absorbance of a solution. This method is often used to determine the concentration of a chemical in a solution.
https://orcid.org/0000-0002-0640-0422
The determination of the mass of a gas or vapour adsorbed to a surface.
gravimetric sorption
gravimetric sorption-desorption
gravimetric sorption-desorption analysis
gravimetric sorption/desorption
gravimetric sorption/desorption analysis
CHMO:0000002
gravimetric sorption analysis
The determination of the mass of a gas or vapour adsorbed to a surface.
https://orcid.org/0000-0002-0640-0422
The use of an electrochemical cell to measure a qualitative or quantitative response.
FIX:0000764
electroanalytical method
electrochemical assay
electrochemical method
CHMO:0000003
electrochemical analysis
The use of an electrochemical cell to measure a qualitative or quantitative response.
FIX:0000764
OrangeBook:8.1
An electrochemical technique where the cell current is measured whilst the potential difference between the indicator and reference electrodes is controlled.
amperometric method
CHMO:0000004
amperometry
An electrochemical technique where the cell current is measured whilst the potential difference between the indicator and reference electrodes is controlled.
FIX:0000783
OrangeBook:8.5.2
An electrochemical technique where the time dependence of the cell current is measured whilst the potential difference between the indicator and reference electrodes is controlled.
chronoamperometry
CHMO:0000005
chrono-amperometry
An electrochemical technique where the time dependence of the cell current is measured whilst the potential difference between the indicator and reference electrodes is controlled.
FIX:0000785
OrangeBook:8.5.2
An electrochemical technique where the time dependence of the cell current is measured whilst the potential difference between the indicator and reference electrodes is controlled. Measurements are taken every 1 to 5 s.
high-speed chronoamperometry
CHMO:0000006
high-speed chrono-amperometry
An electrochemical technique where the time dependence of the cell current is measured whilst the potential difference between the indicator and reference electrodes is controlled. Measurements are taken every 1 to 5 s.
https://doi.org/10.1373/49.10.1763
An electrochemical technique where the time dependence of the cell current is measured whilst the potential difference between the indicator and reference electrodes is varied as a step function.
potential step chronoamperometry
CHMO:0000007
potential step chrono-amperometry
An electrochemical technique where the time dependence of the cell current is measured whilst the potential difference between the indicator and reference electrodes is varied as a step function.
https://doi.org/10.1039/b816223a
An electrochemical technique where the cell current is measured whilst the potential difference between the indicator and reference electrodes is held at a constant value (sufficient to oxidize or reduce the sample).
CPA
constant-potential amperometry
CHMO:0000008
constant potential amperometry
An electrochemical technique where the cell current is measured whilst the potential difference between the indicator and reference electrodes is held at a constant value (sufficient to oxidize or reduce the sample).
https://doi.org/10.1373/49.10.1763
An electrochemical technique where the cell direct current is measured whilst the potential difference between the indicator and reference electrodes is controlled.
DC amperometry
dc amperometry
direct-current amperometry
CHMO:0000009
direct current amperometry
An electrochemical technique where the cell direct current is measured whilst the potential difference between the indicator and reference electrodes is controlled.
https://doi.org/10.1039/b816289a
The measurement of the conductance of a solution as a function of concentration. Measurements are made indirectly across the resistance of the solution with alternating current.
FIX:0000768
FIX:0000770
conductimetry
CHMO:0000010
conductometry
The measurement of the conductance of a solution as a function of concentration. Measurements are made indirectly across the resistance of the solution with alternating current.
Orange:8.5.4
The measurement of the conductance of a solution as a function of concentration. Measurements are made indirectly across the resistance of the solution with high-frequency alternating current (>0.1 MHz).
FIX:0000773
high frequency conductimetry
high frequency conductometry
CHMO:0000011
high-frequency conductometry
The measurement of the conductance of a solution as a function of concentration. Measurements are made indirectly across the resistance of the solution with high-frequency alternating current (>0.1 MHz).
https://orcid.org/0000-0002-0640-0422
An electrochemical technique where the total Coulombs of electricity required to complete (fully oxidise or fully reduce the sample in) an electrochemical reaction is measured.
CHMO:0000012
coulometry
An electrochemical technique where the total Coulombs of electricity required to complete (fully oxidise or fully reduce the sample in) an electrochemical reaction is measured.
Orange:8.5.1
An electrochemical technique where the total Coulombs of electricity required to complete (fully oxidise or fully reduce the sample in) an electrochemical reaction is measured whilst the current is held at a constant value.
controlled current coulometry
controlled-current coulometry
CHMO:0000013
amperostatic coulometry
An electrochemical technique where the total Coulombs of electricity required to complete (fully oxidise or fully reduce the sample in) an electrochemical reaction is measured whilst the current is held at a constant value.
OrangeBook:8.5.1
An electrochemical technique where the time-dependence of the total Coulombs of electricity required to complete (fully oxidise or fully reduce the sample in) an electrochemical reaction is measured whilst the current is held at a constant value.
chronocoulometry
CHMO:0000014
chrono-coulometry
An electrochemical technique where the time-dependence of the total Coulombs of electricity required to complete (fully oxidise or fully reduce the sample in) an electrochemical reaction is measured whilst the current is held at a constant value.
FIX:0000786
https://orcid.org/0000-0002-0640-0422
An electrochemical technique where the total Coulombs of electricity required to complete (fully oxidise or fully reduce the sample in) an electrochemical reaction is measured whilst the potential of the working electrode is held at a constant value.
bulk electrolysis
controlled potential coulometry
controlled-potential coulometry
CHMO:0000015
potentiostatic coulometry
An electrochemical technique where the total Coulombs of electricity required to complete (fully oxidise or fully reduce the sample in) an electrochemical reaction is measured whilst the potential of the working electrode is held at a constant value.
FIX:0000787
OrangeBook:8.5.2
An electrochemical technique where the potential difference between the indicator and reference electrodes is measured under conditions where the current passed is sufficiently small to maintain thermodynamic equilibrium.
potentiometric method
CHMO:0000016
potentiometry
An electrochemical technique where the potential difference between the indicator and reference electrodes is measured under conditions where the current passed is sufficiently small to maintain thermodynamic equilibrium.
FIX:0000775
OrangeBook:8.5.1
An electrochemical technique where the time-dependence of the potential difference between the indicator and reference electrodes is measured under conditions where the current passed is sufficiently small to maintain thermodynamic equilibrium.
chronopotentiometry
CHMO:0000017
chrono-potentiometry
An electrochemical technique where the time-dependence of the potential difference between the indicator and reference electrodes is measured under conditions where the current passed is sufficiently small to maintain thermodynamic equilibrium.
FIX:0000780
OrangeBook:8.5.1
An electrochemical technique where the analyte of interest is electroplated onto the working electrode before being removed or 'stripped'. During removal the time-dependence of the potential difference between the indicator and reference electrodes is measured under conditions where the current passed is sufficiently small to maintain thermodynamic equilibrium.
chronopotentiometric stripping
SP
CHMO:0000018
stripping potentiometry
An electrochemical technique where the analyte of interest is electroplated onto the working electrode before being removed or 'stripped'. During removal the time-dependence of the potential difference between the indicator and reference electrodes is measured under conditions where the current passed is sufficiently small to maintain thermodynamic equilibrium.
https://doi.org/10.1016/j.talanta.2004.07.034
SP
An electrochemical technique where the analyte of interest is electroplated onto the working electrode before being removed or 'stripped' by re-oxidation using either oxidants in the sample or by applying a small constant current, or a combination of both. During removal the time-dependence of the potential difference between the indicator and reference electrodes is measured under conditions where the current passed is sufficiently small to maintain thermodynamic equilibrium.
ASP
anodic-stripping voltammetry
CHMO:0000019
anodic stripping potentiometry
An electrochemical technique where the analyte of interest is electroplated onto the working electrode before being removed or 'stripped' by re-oxidation using either oxidants in the sample or by applying a small constant current, or a combination of both. During removal the time-dependence of the potential difference between the indicator and reference electrodes is measured under conditions where the current passed is sufficiently small to maintain thermodynamic equilibrium.
https://doi.org/10.1016/j.talanta.2004.07.034
An electrochemical technique where the analyte of interest is electroplated onto the working electrode before being removed or 'stripped' by re-reduction. During removal the time-dependence of the potential difference between the indicator and reference electrodes is measured under conditions where the current passed is sufficiently small to maintain thermodynamic equilibrium.
CSP
cathodic-stripping voltammetry
CHMO:0000020
cathodic stripping potentiometry
An electrochemical technique where the analyte of interest is electroplated onto the working electrode before being removed or 'stripped' by re-reduction. During removal the time-dependence of the potential difference between the indicator and reference electrodes is measured under conditions where the current passed is sufficiently small to maintain thermodynamic equilibrium.
https://doi.org/10.1016/j.talanta.2004.07.034
An electrochemical technique where the potential difference between the indicator and reference electrodes is measured under conditions where the current passed is sufficiently small to maintain thermodynamic equilibrium and held at a constant (non-zero) value.
controlled current potentiometry
CHMO:0000021
controlled-current potentiometry
An electrochemical technique where the potential difference between the indicator and reference electrodes is measured under conditions where the current passed is sufficiently small to maintain thermodynamic equilibrium and held at a constant (non-zero) value.
FIX:0000778
OrangeBook:8.5.1
An electrochemical technique where the potential difference between an ion-selective indicator electrode and the reference electrode is measured under conditions where the current passed is sufficiently small to maintain thermodynamic equilibrium.
CHMO:0000022
ion-selective potentiometry
An electrochemical technique where the potential difference between an ion-selective indicator electrode and the reference electrode is measured under conditions where the current passed is sufficiently small to maintain thermodynamic equilibrium.
https://orcid.org/0000-0002-0640-0422
An *obsolete* electrochemical technique where the potential difference between the indicator and reference electrodes is measured using an oscillograph under conditions where the current passed is sufficiently small to maintain thermodynamic equilibrium.
oscillo potentiometry
CHMO:0000023
oscillographic potentiometry
An *obsolete* electrochemical technique where the potential difference between the indicator and reference electrodes is measured using an oscillograph under conditions where the current passed is sufficiently small to maintain thermodynamic equilibrium.
https://orcid.org/0000-0002-0640-0422
An electrochemical technique where the cell current is measured as a function of time and as a function of the potential between the indicator and reference electrodes.
voltammetric method
CHMO:0000024
voltammetry
An electrochemical technique where the cell current is measured as a function of time and as a function of the potential between the indicator and reference electrodes.
FIX:0000765
OrangeBook:8.5.3
An electrochemical technique where the cell current is measured as a function of time and as a function of the potential between the indicator and reference electrodes. The potential is varied linearly and inverts at the end point resulting in a cycle.
cyclic triangular wave voltammetry
cyclovoltammetry
CV
CHMO:0000025
cyclic voltammetry
An electrochemical technique where the cell current is measured as a function of time and as a function of the potential between the indicator and reference electrodes. The potential is varied linearly and inverts at the end point resulting in a cycle.
FIX:0000099
OrangeBook:8.5.3
CV
An electrochemical technique where the cell current is measured as a function of time and as a function of the potential between the indicator and reference electrodes. The potential is varied linearly and inverts at the end point resulting in a cycle which repeats approximately every 100 ms.
FCV
FSCV
fast cyclic voltammetry
fast scan cyclic voltammetry
CHMO:0000026
fast-scan cyclic voltammetry
An electrochemical technique where the cell current is measured as a function of time and as a function of the potential between the indicator and reference electrodes. The potential is varied linearly and inverts at the end point resulting in a cycle which repeats approximately every 100 ms.
FIX:0000761
https://doi.org/10.1373/49.10.1763
An electrochemical technique where the cell current flowing during convective mass transfer (the movement of material by the action of a fluid) is measured as a function of time and as a function of the potential between the indicator and reference electrodes. The potential is varied linearly and inverts at the end point resulting in a cycle.
linear scan hydrodynamic voltammetry
linear-scan hydrodynamic voltammetry
CHMO:0000027
hydrodynamic voltammetry
An electrochemical technique where the cell current flowing during convective mass transfer (the movement of material by the action of a fluid) is measured as a function of time and as a function of the potential between the indicator and reference electrodes. The potential is varied linearly and inverts at the end point resulting in a cycle.
FIX:0000792
Orange: 8.5.3
An electrochemical technique where the cell current is measured as a function of time and as a function of the potential between the indicator and reference electrodes. The potential is varied linearly and stops at an end point.
LSV
chrono amperometry with linear potenial sweep
chronoamperometry with linear sweep
electrode voltammetry
linear sweep voltammetry
stationary electrode voltammetry
CHMO:0000028
linear-sweep voltammetry
An electrochemical technique where the cell current is measured as a function of time and as a function of the potential between the indicator and reference electrodes. The potential is varied linearly and stops at an end point.
FIX:0000791
OrangeBook:8.5.3
An electrochemical technique where the cell current is measured as a function of time and as a function of the potential between the indicator and reference electrodes. The potential is varied using pulses of increasing amplitude.
CHMO:0000029
pulse voltammetry
An electrochemical technique where the cell current is measured as a function of time and as a function of the potential between the indicator and reference electrodes. The potential is varied using pulses of increasing amplitude.
https://orcid.org/0000-0002-0640-0422
An electrochemical technique where the cell current is measured as a function of time and as a function of the potential between the indicator and reference electrodes. The potential is varied using pulses of increasing amplitude and the current is sampled before and after each voltage pulse.
DPV
differential-pulse voltammetry
CHMO:0000030
differential pulse voltammetry
An electrochemical technique where the cell current is measured as a function of time and as a function of the potential between the indicator and reference electrodes. The potential is varied using pulses of increasing amplitude and the current is sampled before and after each voltage pulse.
https://orcid.org/0000-0002-0640-0422
An electrochemical technique where the cell current is measured as a function of time and as a function of the potential between the indicator and reference electrodes. The potential is varied using pulses of increasing amplitude and the current is sampled after each voltage pulse.
NPV
normal-pulse voltammetry
CHMO:0000031
normal pulse voltammetry
An electrochemical technique where the cell current is measured as a function of time and as a function of the potential between the indicator and reference electrodes. The potential is varied using pulses of increasing amplitude and the current is sampled after each voltage pulse.
ISBN:978-3-540-74597-6
An electrochemical technique where the cell current is measured as a function of time and as a function of the potential between the indicator and reference electrodes. The working electrode is a dropping mercury (or other liquid conductor) electrode and unstirred solutions are used.
CHMO:0000032
polarography
An electrochemical technique where the cell current is measured as a function of time and as a function of the potential between the indicator and reference electrodes. The working electrode is a dropping mercury (or other liquid conductor) electrode and unstirred solutions are used.
FIX:0000794
OrangeBook:8.5.3
An electrochemical technique where the alternating current (ac) component of the cell current is measured as a function of time and as a function of the ac potential between the indicator and reference electrodes. The working electrode is a dropping mercury (or other liquid conductor) electrode and unstirred solutions are used.
AC polarography
AC-polarography
alternating-current polarography
CHMO:0000033
alternating current polarography
An electrochemical technique where the alternating current (ac) component of the cell current is measured as a function of time and as a function of the ac potential between the indicator and reference electrodes. The working electrode is a dropping mercury (or other liquid conductor) electrode and unstirred solutions are used.
FIX:0000814
OrangeBook:8.5.3
An electrochemical technique where the ac component of the cell current is measured as a function of time and as a function of the ac potential between the indicator and reference electrodes. The working electrode is a dropping mercury (or other liquid conductor) electrode and unstirred solutions are used. The cell current is sampled on alternate half cycles and the potential is applied as a small amplitude square wave superimposed on a linear sweep.
CHMO:0000034
Kalousek polarography
An electrochemical technique where the ac component of the cell current is measured as a function of time and as a function of the ac potential between the indicator and reference electrodes. The working electrode is a dropping mercury (or other liquid conductor) electrode and unstirred solutions are used. The cell current is sampled on alternate half cycles and the potential is applied as a small amplitude square wave superimposed on a linear sweep.
https://doi.org/10.1080/10408348508542784
An electrochemical technique where the ac component of the cell current is measured as a function of time and as a function of the ac potential between the indicator and reference electrodes. The working electrode is a dropping mercury (or other liquid conductor) electrode and unstirred solutions are used. The cell current is sampled (only once per drop lifetime) on alternate half cycles and the potential is applied as a large amplitude square wave superimposed on a linear sweep.
square wave polarography
CHMO:0000035
square-wave polarography
An electrochemical technique where the ac component of the cell current is measured as a function of time and as a function of the ac potential between the indicator and reference electrodes. The working electrode is a dropping mercury (or other liquid conductor) electrode and unstirred solutions are used. The cell current is sampled (only once per drop lifetime) on alternate half cycles and the potential is applied as a large amplitude square wave superimposed on a linear sweep.
FIX:0000816
OrangeBook:8.5.3
An electrochemical technique where the cell current is measured as a function of time and as a function of the potential between the indicator and reference electrodes. The working electrode is a dropping mercury (or other liquid conductor) electrode and unstirred solutions are used. The potential is varied using pulses of linearly increasing amplitude (one pulse during each drop lifetime) and the current is sampled before and after each voltage pulse.
CHMO:0000036
differential pulse polarography
An electrochemical technique where the cell current is measured as a function of time and as a function of the potential between the indicator and reference electrodes. The working electrode is a dropping mercury (or other liquid conductor) electrode and unstirred solutions are used. The potential is varied using pulses of linearly increasing amplitude (one pulse during each drop lifetime) and the current is sampled before and after each voltage pulse.
FIX:0000813
https://orcid.org/0000-0002-0640-0422
An electrochemical technique where the cell current is measured as a function of time and as a function of the potential between the indicator and reference electrodes. The working electrode is a dropping mercury (or other liquid conductor) electrode and unstirred solutions are used. The potential is varied using pulses of linearly increasing amplitude (one pulse during each drop lifetime) and the current is sampled after each voltage pulse.
CHMO:0000037
normal pulse polarography
An electrochemical technique where the cell current is measured as a function of time and as a function of the potential between the indicator and reference electrodes. The working electrode is a dropping mercury (or other liquid conductor) electrode and unstirred solutions are used. The potential is varied using pulses of linearly increasing amplitude (one pulse during each drop lifetime) and the current is sampled after each voltage pulse.
FIX:0000812
https://orcid.org/0000-0002-0640-0422
An *obsolete* electrochemical technique where the cell current is measured as a function of time and as a function of the potential between the indicator and reference electrodes using an oscillograph. The working electrode is a dropping mercury (or other liquid conductor) electrode and unstirred solutions are used.
oscillo-polography
oscillopolography
CHMO:0000038
oscillo polarography
An *obsolete* electrochemical technique where the cell current is measured as a function of time and as a function of the potential between the indicator and reference electrodes using an oscillograph. The working electrode is a dropping mercury (or other liquid conductor) electrode and unstirred solutions are used.
ISBN:978-3-540-74597-6
An electrochemical technique where the cell current is measured as a function of time and as a function of the potential between the indicator and reference electrodes. The working electrode is a dropping mercury (or other liquid conductor) electrode and unstirred solutions are used. The current is sampled only during a specific time interval of the life of each drop of the droppping mercury electrode.
CHMO:0000039
tast polarography
An electrochemical technique where the cell current is measured as a function of time and as a function of the potential between the indicator and reference electrodes. The working electrode is a dropping mercury (or other liquid conductor) electrode and unstirred solutions are used. The current is sampled only during a specific time interval of the life of each drop of the droppping mercury electrode.
FIX:0000795
OrangeBook:8.5.3
An electrochemical technique where the cell current is measured as a function of time and as a function of the potential between the indicator and reference electrodes. The potential is varied as a square wave and the current is measured at the end of each half-wave, just prior to potential change.
SWV
square wave voltammetry
CHMO:0000040
square-wave voltammetry
An electrochemical technique where the cell current is measured as a function of time and as a function of the potential between the indicator and reference electrodes. The potential is varied as a square wave and the current is measured at the end of each half-wave, just prior to potential change.
FIX:0000816
https://orcid.org/0000-0002-0640-0422
An electrochemical technique where the analyte of interest is first deposited (usually by electroplating) onto the working electrode before being removed or 'stripped'. During removal the cell current is measured as a function of time and as a function of the potential between the indicator and reference electrodes.
SV
CHMO:0000041
stripping voltammetry
An electrochemical technique where the analyte of interest is first deposited (usually by electroplating) onto the working electrode before being removed or 'stripped'. During removal the cell current is measured as a function of time and as a function of the potential between the indicator and reference electrodes.
https://orcid.org/0000-0002-0640-0422
An electrochemical technique where the analyte of interest is first electroplated onto the working electrode before being removed or 'stripped' by applying an oxidising potential. During removal the cell current is measured as a function of time and as a function of the potential between the indicator and reference electrodes.
ASV
CHMO:0000042
anodic stripping voltammetry
An electrochemical technique where the analyte of interest is first electroplated onto the working electrode before being removed or 'stripped' by applying an oxidising potential. During removal the cell current is measured as a function of time and as a function of the potential between the indicator and reference electrodes.
https://orcid.org/0000-0002-0640-0422
An electrochemical technique where the analyte of interest is first electroplated onto the working electrode before being removed or 'stripped' by applying an oxidising potential (as a series of voltage pulses of increasing amplitude). During removal the cell current is measured as a function of time and as a function of the potential between the indicator and reference electrodes. The current is sampled before and after each voltage pulse.
DPASV
CHMO:0000043
differential pulse anodic stripping voltammetry
An electrochemical technique where the analyte of interest is first electroplated onto the working electrode before being removed or 'stripped' by applying an oxidising potential (as a series of voltage pulses of increasing amplitude). During removal the cell current is measured as a function of time and as a function of the potential between the indicator and reference electrodes. The current is sampled before and after each voltage pulse.
https://orcid.org/0000-0002-0640-0422
An electrochemical technique where the analyte of interest is first electroplated onto the working electrode before being removed or 'stripped' by applying an oxidising potential. During removal the cell current is measured as a function of time and as a function of the potential between the indicator and reference electrodes. A plot of stripping peak current versus deposition potential resembles a polarogram.
pseudo-polarography
pseudopolarography
CHMO:0000044
pseudo polarography
An electrochemical technique where the analyte of interest is first electroplated onto the working electrode before being removed or 'stripped' by applying an oxidising potential. During removal the cell current is measured as a function of time and as a function of the potential between the indicator and reference electrodes. A plot of stripping peak current versus deposition potential resembles a polarogram.
ISBN:978-3-540-74597-6
An electrochemical technique where the analyte of interest is first electroplated onto the working electrode before being removed or 'stripped' by applying an oxidising potential. During removal the cell current is measured as a function of time and as a function of the potential between the indicator and reference electrodes. The potential is varied as a square wave superimposed on a linear sweep.
SWASV
square wave anodic stripping voltammetry
square-wave ASV
CHMO:0000045
square-wave anodic stripping voltammetry
An electrochemical technique where the analyte of interest is first electroplated onto the working electrode before being removed or 'stripped' by applying an oxidising potential. During removal the cell current is measured as a function of time and as a function of the potential between the indicator and reference electrodes. The potential is varied as a square wave superimposed on a linear sweep.
https://doi.org/10.1039/b806470k
An electrochemical technique where the analyte of interest is first adsorbed onto the working electrode before being removed or 'stripped'. During removal the cell current is measured as a function of time and as a function of the potential between the indicator and reference electrodes.
AdSV
adsorptive-stripping voltammetry
CHMO:0000046
adsorptive stripping voltammetry
An electrochemical technique where the analyte of interest is first adsorbed onto the working electrode before being removed or 'stripped'. During removal the cell current is measured as a function of time and as a function of the potential between the indicator and reference electrodes.
https://orcid.org/0000-0002-0640-0422
An electrochemical technique where the analyte of interest is first electroplated onto the working electrode before being removed or 'stripped' by applying a reducing potential. During removal the cell current is measured as a function of time and as a function of the potential between the indicator and reference electrodes.
CSV
CHMO:0000047
cathodic stripping voltammetry
An electrochemical technique where the analyte of interest is first electroplated onto the working electrode before being removed or 'stripped' by applying a reducing potential. During removal the cell current is measured as a function of time and as a function of the potential between the indicator and reference electrodes.
https://orcid.org/0000-0002-0640-0422
true
The simultaneous measurement of spectra and images. A radiation source illuminates the sample and a series of spatially resolved spectra are collected.
CIS
chemical imaging spectrometry
chemical imaging spectroscopy
hyperspectral imaging
imaging spectrometry
imaging spectroscopy
multispectral imaging
spectral imaging
spectroscopic imaging
CHMO:0000049
chemical imaging
The simultaneous measurement of spectra and images. A radiation source illuminates the sample and a series of spatially resolved spectra are collected.
https://orcid.org/0000-0002-0640-0422
The collection of spatially resolved infrared spectra of a sample during optical microscopy.
CHMO:0000583
IR microscopy
IR spectromicroscopy
IR-MSP
IRI
infra-red chemical imaging spectrometry
infra-red microscopy
infrared chemical imaging spectrometry
infrared chemical imaging spectroscopy
infrared mapping
infrared microspectrophotometry
infrared microspectroscopy
infrared spectromicroscopy
CHMO:0000050
infrared microscopy
The collection of spatially resolved infrared spectra of a sample during optical microscopy.
FIX:0000696
ISBN:2884490736
The collection of spatially resolved infrared spectra of a sample during optical microscopy. The infrared spectra are obtained by single pulse of infrared radiation, and are subject to a Fourier transform.
CHMO:0000584
FT-IR imaging
FT-IR microscopy
FTIR imaging
FTIR microscopy
FTIR microspectroscopy
FTIR spectromicroscopy
FTIR-MSP
Fourier transform infra-red microspectrometry
Fourier transform infra-red microspectroscopy
Fourier transform infrared microspectrometry
Fourier transform infrared microspectroscopy
Fourier transform infrared spectromicroscopy
Fourier-transform infrared microscopy
CHMO:0000051
Fourier transform infrared microscopy
The collection of spatially resolved infrared spectra of a sample during optical microscopy. The infrared spectra are obtained by single pulse of infrared radiation, and are subject to a Fourier transform.
https://doi.org/10.1039/b805223a
The collection of spatially resolved near-infrared spectra (0.8 to 2 micrometres) of a sample during microscopy.
NIR chemical imaging spectrometry
NIR chemical imaging spectroscopy
NOIM
near infra red chemical imaging spectrometry
near infra red chemical imaging spectroscopy
near infra-red chemical imaging spectrometry
near infra-red chemical imaging spectroscopy
near infra-red microscopy
near infrared microscopy spectroscopy
near infrared optical microscopy
near-IR spectromicroscopy
near-infra-red microscopy
near-infrared microscopy
near-infrared spectromicroscopy
CHMO:0000052
near-infrared microscopy
The collection of spatially resolved near-infrared spectra (0.8 to 2 micrometres) of a sample during microscopy.
FIX:0000699
https://orcid.org/0000-0002-0640-0422
The collection of spatially resolved mass spectra of a sample during microscopy which are used to visualise the spatial distribution of compounds by their molecular masses.
I-MS
IMS
imaging MS
CHMO:0000053
imaging mass spectrometry
The collection of spatially resolved mass spectra of a sample during microscopy which are used to visualise the spatial distribution of compounds by their molecular masses.
https://doi.org/10.1039/b812533c
The collection of spatially resolved mass spectra of a sample during microscopy where a pulse laser is used to produce both ionisation and vapourisation and the sample is held in a matrix (such as dihydrobenzoic acid) to protect it from direct laser illumination and to separate the sample molecules. The spectra are used to visualise the spatial distribution of (typically) biomolecules by their molecular masses.
MALDI-IMS
MALDI-MS imaging
matrix-assisted laser desorption/ionization imaging mass spectroscopy
CHMO:0000054
matrix-assisted laser desorption-ionisation imaging mass spectrometry
The collection of spatially resolved mass spectra of a sample during microscopy where a pulse laser is used to produce both ionisation and vapourisation and the sample is held in a matrix (such as dihydrobenzoic acid) to protect it from direct laser illumination and to separate the sample molecules. The spectra are used to visualise the spatial distribution of (typically) biomolecules by their molecular masses.
https://doi.org/10.1039/b812533c
The collection of spatially resolved mass spectra of a sample during microscopy where the sample is bombarded with a stream of primary mass-selected particles and the secondary ions ejected from the sample are detected. The spectra are used to visualise the spatial distribution of compounds by their molecular masses.
FIX:0000960
SIMS imaging
SIMS microscopy
secondary ion mass spectroscopy imaging
CHMO:0000055
secondary ion mass spectrometry imaging
The collection of spatially resolved mass spectra of a sample during microscopy where the sample is bombarded with a stream of primary mass-selected particles and the secondary ions ejected from the sample are detected. The spectra are used to visualise the spatial distribution of compounds by their molecular masses.
https://orcid.org/0000-0002-0640-0422
The collection of spatially resolved Raman spectra of a sample during optical microscopy.
CHMO:0000673
FIX:0000697
LRMA
MRS
RCIS
Raman chemical imaging spectrometry
Raman chemical imaging spectroscopy
Raman imaging
Raman mapping
Raman micro spectrometry
Raman micro spectroscopy
Raman microprobe spectroscopy
Raman microspectrometry
Raman microspectroscopy
Raman spectral imaging
laser Raman microanalysis
micro Raman spectrometry
micro Raman spectroscopy
micro-Raman spectrometry
micro-Raman spectroscopy
CHMO:0000056
Raman microscopy
The collection of spatially resolved Raman spectra of a sample during optical microscopy.
https://doi.org/10.1039/b815117b
The detection of luminescence from a sample.
FIX:0000427
CHMO:0000057
luminescence detection
The detection of luminescence from a sample.
https://orcid.org/0000-0002-0640-0422
The detection of luminescence emitted from a sample as a result of a chemical reaction.
CL detection
CHMO:0000058
chemiluminescence detection
The detection of luminescence emitted from a sample as a result of a chemical reaction.
https://doi.org/10.1039/b812750f
The detection of chemiluminescence caused the emission of light by tiny bubbles in a liquid excited by sound.
SCL detection
sono chemiluminescence detection
sono-chemiluminescence detection
sonodynamic chemiluminescence detection
CHMO:0000059
sonochemiluminescence detection
The detection of chemiluminescence caused the emission of light by tiny bubbles in a liquid excited by sound.
https://doi.org/10.1039/b813330a
The measurement or detection of luminescence which results from the molecular absorption of a photon which triggers the emission of a photon with a longer wavelength.
fluorescence (FL) detection
CHMO:0000060
fluorescence detection
The measurement or detection of luminescence which results from the molecular absorption of a photon which triggers the emission of a photon with a longer wavelength.
FIX:0000421
https://orcid.org/0000-0002-0640-0422
A method for analysing microscopic particles suspended in a stream of fluid. The particles are individually passed through a laser beam and the resulting fluorescence and scattered light is detected.
flow cytometric analysis
flow cytometric studies
CHMO:0000061
flow cytometry
A method for analysing microscopic particles suspended in a stream of fluid. The particles are individually passed through a laser beam and the resulting fluorescence and scattered light is detected.
https://orcid.org/0000-0002-0640-0422
A method for determining the distance between molecules using an energy transfer between two chromophores (a donor and an acceptor) in close proximity (typically <10 nm) via a nonradiative, long-range dipole-dipole coupling mechanism.
Forster resonant energy transfer
Förster resonance energy transfer
FRET
CHMO:0000062
Forster resonance energy transfer
A method for determining the distance between molecules using an energy transfer between two chromophores (a donor and an acceptor) in close proximity (typically <10 nm) via a nonradiative, long-range dipole-dipole coupling mechanism.
https://orcid.org/0000-0002-0640-0422
FRET
Forster resonance energy transfer in a bioluminescent system, usually between a luciferase (donor) and a green fluorescent protein (acceptor).
BRET
CHMO:0000063
The luciferase is bioluminescent therefore external illumination is not required.
bioluminescence resonance energy transfer
Forster resonance energy transfer in a bioluminescent system, usually between a luciferase (donor) and a green fluorescent protein (acceptor).
https://orcid.org/0000-0002-0640-0422
A method for determining the distance between molecules using an energy transfer between two fluorescent chromophores (a donor and an acceptor) in close proximity (typically <10 nm) via a nonradiative, long-range dipole-dipole coupling mechanism. Energy transfer usually occurs between a cyan fluorescent protein (donor) and a yellow fluorescent protein (acceptor).
FIX:0000472
FIX:0000473
fluorescence resonance energy transfer assay
fluorescence resonance energy transfer microscopy
fluorescent resonance energy transfer
FRET
CHMO:0000064
fluorescence resonance energy transfer
A method for determining the distance between molecules using an energy transfer between two fluorescent chromophores (a donor and an acceptor) in close proximity (typically <10 nm) via a nonradiative, long-range dipole-dipole coupling mechanism. Energy transfer usually occurs between a cyan fluorescent protein (donor) and a yellow fluorescent protein (acceptor).
https://orcid.org/0000-0002-0640-0422
FRET
A method for determining the mobility of fluorescent molecules by photobleaching a sub-set of the sample during fluorescence microscopy and monitoring the movement of the remaining fluorescent molecules.
FRAP
CHMO:0000065
fluorescence recovery after photobleaching
A method for determining the mobility of fluorescent molecules by photobleaching a sub-set of the sample during fluorescence microscopy and monitoring the movement of the remaining fluorescent molecules.
https://orcid.org/0000-0002-0640-0422
The measurement of the fluorescence decay time of probes solubilised in micellar surfactant solutions in the presence of quenchers.
TRFQ
TRFQ analysis
TRFQ measurements
TRFQ spectrometry
TRFQ spectroscopy
time resolved fluorescence quenching
time resolved fluorescence quenching spectrometry
time-resolved fluorescence quenching spectrometry
time-resolved fluorescence quenching spectroscopy
CHMO:0000066
time-resolved fluorescence quenching
The measurement of the fluorescence decay time of probes solubilised in micellar surfactant solutions in the presence of quenchers.
https://doi.org/10.1039/b813498g
Any technique where a microscope is used to view a small object (or specimen) by producing a magnified image.
FIX:0000005
CHMO:0000067
microscopy
Any technique where a microscope is used to view a small object (or specimen) by producing a magnified image.
https://orcid.org/0000-0002-0640-0422
Microscopy where the specimen is bombarded with a finely focused (<10 nm diameter) electron beam with an acceleration voltage 50-150 kV under vacuum. The interaction of the electrons with the specimen produces transmitted, secondary, backscattered and diffracted electrons and characteristic X-rays which are detected.
FIX:0000051
EM
CHMO:0000068
electron microscopy
Microscopy where the specimen is bombarded with a finely focused (<10 nm diameter) electron beam with an acceleration voltage 50-150 kV under vacuum. The interaction of the electrons with the specimen produces transmitted, secondary, backscattered and diffracted electrons and characteristic X-rays which are detected.
https://doi.org/10.1351/goldbook.S05484
Microscopy where the specimen is bombarded with a finely focused (<10 nm diameter) electron beam produced by field emission with an acceleration voltage 50-150 kV under vacuum. The interaction of the electrons with the specimen produces transmitted, secondary, backscattered and diffracted electrons and characteristic X-rays which are detected.
FEM
field electron microscopy
field emission electron microscopy
field emission microscopy
field-emission microscopy
CHMO:0000069
field-emission electron microscopy
Microscopy where the specimen is bombarded with a finely focused (<10 nm diameter) electron beam produced by field emission with an acceleration voltage 50-150 kV under vacuum. The interaction of the electrons with the specimen produces transmitted, secondary, backscattered and diffracted electrons and characteristic X-rays which are detected.
Orange:17.2.7
Microscopy where the specimen is bombarded with a finely focused (<10 nm diameter) low energy (1-100 eV) electron beam with an acceleration voltage 50-150 kV under vacuum. The interaction of the electrons with the specimen produces transmitted, secondary, backscattered and diffracted electrons and characteristic X-rays which are detected.
LE EM
LEEM
low energy EM
low energy electron microscopy
low-energy EM
CHMO:0000070
low-energy electron microscopy
Microscopy where the specimen is bombarded with a finely focused (<10 nm diameter) low energy (1-100 eV) electron beam with an acceleration voltage 50-150 kV under vacuum. The interaction of the electrons with the specimen produces transmitted, secondary, backscattered and diffracted electrons and characteristic X-rays which are detected.
https://orcid.org/0000-0002-0640-0422
Low-energy electron microscopy where a magnet is used to align all electron spins parallel to the sample surface.
SPLEEM
spin polarised LEEM
spin polarised low energy electron microscopy
spin polarized LEEM
spin-polarised LEEM
spin-polarised low-energy electron microscopy
spin-polarized LEEM
spin-polarized low-energy electron microscopy
CHMO:0000071
spin-polarised low energy electron microscopy
Low-energy electron microscopy where a magnet is used to align all electron spins parallel to the sample surface.
https://orcid.org/0000-0002-0640-0422
Microscopy where the specimen is bombarded with a finely focused (<10 nm diameter) electron beam with an acceleration voltage 50-150 kV under vacuum. The electrons elastically scattered by the specimen are detected.
REM
reflection EM
CHMO:0000072
reflection electron microscopy
Microscopy where the specimen is bombarded with a finely focused (<10 nm diameter) electron beam with an acceleration voltage 50-150 kV under vacuum. The electrons elastically scattered by the specimen are detected.
https://orcid.org/0000-0002-0640-0422
Microscopy where a finely focused (<10 nm diameter) electron beam with an acceleration voltage 50-150 kV is scanned across the specimen under vacuum and the interaction of the electrons with the specimen is determined.
FIX:0000124
SEM
scanning electronic microscopy
CHMO:0000073
scanning electron microscopy
Microscopy where a finely focused (<10 nm diameter) electron beam with an acceleration voltage 50-150 kV is scanned across the specimen under vacuum and the interaction of the electrons with the specimen is determined.
https://doi.org/10.1351/goldbook.S05484
Microscopy where a finely focused (<10 nm diameter) electron beam produced by thermionic emission heating (field emission) and with an acceleration voltage 50-150 kV is scanned across the specimen under vacuum and the interaction of the electrons with the specimen is determined.
FE SEM
FE-SEM
FE/SEM
FEG-SEM
FEGSEM
FESEM
FSEM
field emission gun scanning electron microscopy
field emission scanning electron microscopy
field-emission gun scanning electron microscopy
CHMO:0000074
field-emission scanning electron microscopy
Microscopy where a finely focused (<10 nm diameter) electron beam produced by thermionic emission heating (field emission) and with an acceleration voltage 50-150 kV is scanned across the specimen under vacuum and the interaction of the electrons with the specimen is determined.
https://doi.org/10.1039/b818058j
Microscopy where a finely focused (<10 nm diameter) electron beam produced by applying a high voltage to a tungsten crystal (cold-field emission) and with an acceleration voltage 50-150 kV is scanned across the specimen under vacuum and the interaction of the electrons with the specimen is determined.
CFE SEM
CFE-SEM
CFE/SEM
CFEG-SEM
CFEGSEM
CFSEM
cold field emission gun scanning electron microscopy
cold field emission scanning electron microscopy
cold-field-emission gun scanning electron microscopy
cold-field-emission scanning electron microscopy
cold-field-gun scanning electron microscopy
CHMO:0000075
cold-field-emission scanning electron microscopy
Microscopy where a finely focused (<10 nm diameter) electron beam produced by applying a high voltage to a tungsten crystal (cold-field emission) and with an acceleration voltage 50-150 kV is scanned across the specimen under vacuum and the interaction of the electrons with the specimen is determined.
ISBN:0763701920
Microscopy where a finely focused (<10 nm diameter) electron beam with an acceleration voltage 50-150 kV is scanned across the specimen in a gaseous environment and the interaction of the electrons with the specimen is determined.
E-SEM
ESEM
environmental SEM
CHMO:0000076
environmental scanning electron microscopy
Microscopy where a finely focused (<10 nm diameter) electron beam with an acceleration voltage 50-150 kV is scanned across the specimen in a gaseous environment and the interaction of the electrons with the specimen is determined.
https://orcid.org/0000-0002-0640-0422
Microscopy where a finely focused (<10 nm diameter) electron beam with an acceleration voltage 50-150 kV is scanned across the specimen under vacuum. The interaction of electrons with the specimen produces X-rays (with energies characteristic of atomic number) which are detected as a function of wavelength.
SEM EDX
SEM-EDX
SEM-EDXA
SEM/EDX
SEM/EDXA
scanning electron microscopy-energy dispersive X-ray spectroscopy
scanning electron microscopy/energy dispersive X-ray analysis
scanning electron microscopy/energy dispersive X-ray spectroscopy
CHMO:0000077
scanning electron microscopy energy dispersive X-ray spectroscopy
Microscopy where a finely focused (<10 nm diameter) electron beam with an acceleration voltage 50-150 kV is scanned across the specimen under vacuum. The interaction of electrons with the specimen produces X-rays (with energies characteristic of atomic number) which are detected as a function of wavelength.
https://orcid.org/0000-0002-0640-0422
Microscopy where a pulsed electron beam is scanned over the surface of the specimen in order to generate elastic waves which are reflected and detected.
SEAM
CHMO:0000078
scanning electron acoustic microscopy
Microscopy where a pulsed electron beam is scanned over the surface of the specimen in order to generate elastic waves which are reflected and detected.
https://doi.org/10.1007/s10853-005-7244-2
Microscopy where a focused electron beam of small diameter is used to produce Auger electrons which are detected.
scanning Auger electron microscopy
SAM
CHMO:0000079
scanning Auger microscopy
Microscopy where a focused electron beam of small diameter is used to produce Auger electrons which are detected.
https://orcid.org/0000-0002-0640-0422
SAM
Electron microscopy where the intensities of the electrons through an electron-transparent specimen are measured.
FIX:0000126
TEM
CHMO:0000080
transmission electron microscopy
Electron microscopy where the intensities of the electrons through an electron-transparent specimen are measured.
https://doi.org/10.1351/goldbook.T06481
Transmission electron microscopy where the specimen is cooled in liquid ethane to 180 °C.
LT-TEM
cryo TEM
cryo-TEM
cryogenic TEM
low-temperature transmission electron microscopy
CHMO:0000081
cryogenic transmission electron microscopy
Transmission electron microscopy where the specimen is cooled in liquid ethane to 180 °C.
https://doi.org/10.1021/jp013639d
Transmission electron microscopy where the intensities of transmitted electrons of particular kinetic energies are measured.
EF-TEM
EF/TEM
EFTEM
electron spectroscopic imaging
energy filtered TEM
energy filtered transmission electron microscopy
energy-filtered TEM
ESI
CHMO:0000082
energy-filtered transmission electron microscopy
Transmission electron microscopy where the intensities of transmitted electrons of particular kinetic energies are measured.
https://orcid.org/0000-0002-0640-0422
ESI
Transmission electron microscopy where the electron-transparent specimen (normally a fresh tissue or cell suspension) is prepared by rapid freezing using liquid nitrogen, then fractured, and the cold fractured surface is coated with Pt or Au by evaporation.
FF-TEM
FF/TEM
FFTEM
freeze fracture TEM
freeze fracture transmission electron microscopy
freeze-fracture TEM
CHMO:0000083
freeze-fracture transmission electron microscopy
Transmission electron microscopy where the electron-transparent specimen (normally a fresh tissue or cell suspension) is prepared by rapid freezing using liquid nitrogen, then fractured, and the cold fractured surface is coated with Pt or Au by evaporation.
https://doi.org/10.1039/b813498g
Transmission electron microscopy where the phase contrast between the transmitted interfering electron waves is used to produce an image.
HR TEM
HR-TEM
HR/TEM
HRTEM
high resolution (HR) TEM
high resolution TEM
high resolution transmission electron microscopy
high-resolution TEM
phase contrast TEM
phase contrast transmission electron microscopy
phase-contrast TEM
phase-contrast transmission electron microscopy
CHMO:0000084
high-resolution transmission electron microscopy
Transmission electron microscopy where the phase contrast between the transmitted interfering electron waves is used to produce an image.
https://orcid.org/0000-0002-0640-0422
Microscopy where an electron-transparent specimen is bombarded with a finely focused (<10 nm diameter) electron beam with an acceleration voltage 700–3000 kV under vacuum and the intensities of the transmitted electrons are measured.
HV TEM
HV-TEM
HV/TEM
HVTEM
high voltage TEM
high voltage transmission electron microscopy
high-voltage TEM
CHMO:0000085
high-voltage transmission electron microscopy
Microscopy where an electron-transparent specimen is bombarded with a finely focused (<10 nm diameter) electron beam with an acceleration voltage 700–3000 kV under vacuum and the intensities of the transmitted electrons are measured.
https://orcid.org/0000-0002-0640-0422
Microscopy where a finely focused (<10 nm diameter) electron beam with an acceleration voltage 50–150 kV is scanned across an electron-transparent specimen under vacuum and the intensities of the transmitted electrons are measured.
STEM
scanning TEM
CHMO:0000086
scanning transmission electron microscopy
Microscopy where a finely focused (<10 nm diameter) electron beam with an acceleration voltage 50–150 kV is scanned across an electron-transparent specimen under vacuum and the intensities of the transmitted electrons are measured.
https://orcid.org/0000-0002-0640-0422
Any type of microscopy where the specimen can be made to fluoresce (emit energy as visible light) by illuminating it with light of specific wavelengths. These specimens are called fluorophores.
FIX:0000123
FM
fluorescence imaging
fluorescence microscopic imaging
CHMO:0000087
fluorescence microscopy
Any type of microscopy where the specimen can be made to fluoresce (emit energy as visible light) by illuminating it with light of specific wavelengths. These specimens are called fluorophores.
https://orcid.org/0000-0002-0640-0422
Microscopy where the specimen can be made to fluoresce (emit energy as visible light) by scanning a laser spot of specific wavelength over its surface.
FLSM
LSM
laser scanning fluorescence microscopy
laser scanning microscopy
CHMO:0000088
fluorescence laser scanning microscopy
Microscopy where the specimen can be made to fluoresce (emit energy as visible light) by scanning a laser spot of specific wavelength over its surface.
FIX:0000380
https://orcid.org/0000-0002-0640-0422
Microscopy where the specimen can be made to fluoresce (emit energy as visible light) by scanning a gas (Ar or Kr) laser spot of specific wavelength over its surface and using a spatial pinhole to eliminate out-of-focus fluorescence.
CLSM
LSCM
confocal fluorescence imaging
confocal fluorescence microscopy
confocal laser scanning fluorescence microscopy
confocal-laser scanning microscopy
fluorescence confocal microscopy
fluorescence confocal scanning laser microscopy
scanning confocal fluorescence microscopy
CHMO:0000089
confocal laser scanning microscopy
Microscopy where the specimen can be made to fluoresce (emit energy as visible light) by scanning a gas (Ar or Kr) laser spot of specific wavelength over its surface and using a spatial pinhole to eliminate out-of-focus fluorescence.
https://doi.org/10.1039/b807581f
Microscopy where the specimen can be made to fluoresce (emit energy as visible light) by scanning a solid-state (Ti sapphire) laser spot of specific wavelength over its surface to produce multi-photon fluorescence (i.e. the fluorophore simultaneously absorbs multiple photons of typically one half to one third of the energy required for single-photon excitation).
FIX:0000383
MPLSM
multi photon laser scanning microscopy
multiphoton laser scanning microscopy
CHMO:0000090
multi-photon laser scanning microscopy
Microscopy where the specimen can be made to fluoresce (emit energy as visible light) by scanning a solid-state (Ti sapphire) laser spot of specific wavelength over its surface to produce multi-photon fluorescence (i.e. the fluorophore simultaneously absorbs multiple photons of typically one half to one third of the energy required for single-photon excitation).
https://orcid.org/0000-0002-0640-0422
Microscopy where the specimen can be made to fluoresce (emit energy as visible light) by illuminating it with light of specific wavelengths and the spatial distribution of mean fluorescence lifetimes (usually on the ns scale) is mapped within the microscopic images.
FLIM
fluorescence-lifetime imaging microscopy
CHMO:0000091
fluorescence lifetime imaging microscopy
Microscopy where the specimen can be made to fluoresce (emit energy as visible light) by illuminating it with light of specific wavelengths and the spatial distribution of mean fluorescence lifetimes (usually on the ns scale) is mapped within the microscopic images.
https://doi.org/10.1007/b102213
Microscopy where the specimen can be made to fluoresce (emit energy as visible light) by illuminating it with radiation in the infra-red region (2.5–16 μm).
IR fluorescence microscopy
infra-red fluorescence microscopy
CHMO:0000092
infrared fluorescence microscopy
Microscopy where the specimen can be made to fluoresce (emit energy as visible light) by illuminating it with radiation in the infra-red region (2.5–16 μm).
https://orcid.org/0000-0002-0640-0422
Microscopy where the specimen can be made to fluoresce (emit energy as visible light) by illuminating it with radiation in the near infra-red region (0.8–2.5 μm).
NIRF microscopy
NIRFM
near infra-red fluorescence microscopy
near-infrared fluorescence microscopy
CHMO:0000093
near-infrared fluorescence microscopy
Microscopy where the specimen can be made to fluoresce (emit energy as visible light) by illuminating it with radiation in the near infra-red region (0.8–2.5 μm).
https://orcid.org/0000-0002-0640-0422
Microscopy where the specimen (a fluorophore) can be made to fluoresce (emit energy as visible light) by illuminating it with light of specific wavelength. The light is totally internally reflected to generate an evanescent wave at the glass microscope slide-water interface. The evanescent wave selectively illuminates and excites fluorophores in a restricted region of the specimen allowing fluorophores on the surface to be imaged (normally the fluorescence of surface fluorophores is overwhelmed by background fluorescence).
TIRF microscopy
TIRFM
CHMO:0000094
total internal reflection fluorescence microscopy
Microscopy where the specimen (a fluorophore) can be made to fluoresce (emit energy as visible light) by illuminating it with light of specific wavelength. The light is totally internally reflected to generate an evanescent wave at the glass microscope slide-water interface. The evanescent wave selectively illuminates and excites fluorophores in a restricted region of the specimen allowing fluorophores on the surface to be imaged (normally the fluorescence of surface fluorophores is overwhelmed by background fluorescence).
https://orcid.org/0000-0002-0640-0422
Microscopy where the specimen can be made to fluoresce (emit energy as visible light) by illuminating it with radiation in the ultra-violet region (4–380 nm).
UV fluorescence microscopy
UVF microscopy
UVFM
ultra-violet fluorescence microscopy
ultraviolet fluorescence microscopy
CHMO:0000095
ultraviolet fluorescence microscopy
Microscopy where the specimen can be made to fluoresce (emit energy as visible light) by illuminating it with radiation in the ultra-violet region (4–380 nm).
ISBN:0632034335
Microscopy where the specimen can be made to fluoresce (emit energy as visible light) by illuminating it with radiation in the visible region (380–750 nm).
CHMO:0000096
visible fluorescence microscopy
Microscopy where the specimen can be made to fluoresce (emit energy as visible light) by illuminating it with radiation in the visible region (380–750 nm).
https://orcid.org/0000-0002-0640-0422
Microscopy where ions are used to produce an image.
FIX:0000962
IM
CHMO:0000097
ion microscopy
Microscopy where ions are used to produce an image.
https://orcid.org/0000-0002-0640-0422
Microscopy where atoms of an inert gas in the vicinty of the specimen (which is in the form of a very sharp tip <10 m diameter) are ionised by the application of a strong electric field to the tip and an image is produced by the projection of the ions onto a fluorescent screen. The image consists of a pattern of spots of light which correspond to individual atoms on the specimen surface.
FIM
field ionisation microscopy
field ionization microscopy
field-ion microscopy
field-ionisation microscopy
field-ionization microscopy
CHMO:0000098
field ion microscopy
Microscopy where atoms of an inert gas in the vicinty of the specimen (which is in the form of a very sharp tip <10 m diameter) are ionised by the application of a strong electric field to the tip and an image is produced by the projection of the ions onto a fluorescent screen. The image consists of a pattern of spots of light which correspond to individual atoms on the specimen surface.
Orange:17.2.7
Microscopy where atoms in the vicinty of the specimen (which is in the form of a very sharp tip <10 m diameter) are ionised by the application of a strong electric field to the tip and an image is produced by the projection of the ions onto a fluorescent screen. The image consists of a pattern of spots of light which correspond to individual atoms on the specimen surface. When a sudden voltage pulse is applied to the tip, atoms from the surface of the specimen itself are be ejected and travel down a drift tube where their arrival time (a measure of the mass of the atom) can be determined. This allows the atomic composition of the specimen to be determined.
AP FIM
AP field ionisation microscopy
AP field ionization microscopy
AP field-ion microscopy
AP field-ionisation microscopy
AP field-ionization microscopy
AP-FIM
AP/FIM
APFIM
atom probe field ionisation microscopy
atom probe field ionization microscopy
atom probe field-ion microscopy
atom probe field-ionisation microscopy
atom probe field-ionization microscopy
atom-probe field-ion microscopy
CHMO:0000099
atom probe field ion microscopy
Microscopy where atoms in the vicinty of the specimen (which is in the form of a very sharp tip <10 m diameter) are ionised by the application of a strong electric field to the tip and an image is produced by the projection of the ions onto a fluorescent screen. The image consists of a pattern of spots of light which correspond to individual atoms on the specimen surface. When a sudden voltage pulse is applied to the tip, atoms from the surface of the specimen itself are be ejected and travel down a drift tube where their arrival time (a measure of the mass of the atom) can be determined. This allows the atomic composition of the specimen to be determined.
https://orcid.org/0000-0002-0640-0422
Microscopy where atoms of He gas in the vicinty of the specimen are ionised and an image is produced by the projection of the ions onto a fluorescent screen. The image consists of a pattern of spots of light which correspond to individual atoms on the specimen surface.
CHMO:0000100
helium-ion microscopy
Microscopy where atoms of He gas in the vicinty of the specimen are ionised and an image is produced by the projection of the ions onto a fluorescent screen. The image consists of a pattern of spots of light which correspond to individual atoms on the specimen surface.
https://orcid.org/0000-0002-0640-0422
Microscopy where an ion beam is scanned over the specimen surface and the secondary electrons emitted are detected.
FIX:0000963
SIM
CHMO:0000101
scanning ion microscopy
Microscopy where an ion beam is scanned over the specimen surface and the secondary electrons emitted are detected.
https://orcid.org/0000-0002-0640-0422
SIM
Microscopy where the specimen is illuminated with visible light and a system of lenses is used to produce an image.
FIX:0000113
OM
light microscopy
CHMO:0000102
optical microscopy
Microscopy where the specimen is illuminated with visible light and a system of lenses is used to produce an image.
https://orcid.org/0000-0002-0640-0422
Microscopy where visible light coming from the specimen is collected and guided through a pinhole before it is detected. The pinhole allows only light from the focal point to pass to the detector, reducing background interference.
CHMO:0000103
confocal microscopy
Microscopy where visible light coming from the specimen is collected and guided through a pinhole before it is detected. The pinhole allows only light from the focal point to pass to the detector, reducing background interference.
ISBN:978-3-540-74597-6
Microscopy where the specimen is illuminated with light transmitted from a source on the opposite side of the specimen from the objective.
bright field microscopy
bright-field optical microscopy
transmitted light microscopy
transmitted-light microscopy
CHMO:0000104
bright-field microscopy
Microscopy where the specimen is illuminated with light transmitted from a source on the opposite side of the specimen from the objective.
https://orcid.org/0000-0002-0640-0422
Microscopy where two specimens can be compared by illuminating them with visible light using two identical sets of microscope lenses which are linked by an optical bridge.
CHMO:0000105
comparison light microscopy
Microscopy where two specimens can be compared by illuminating them with visible light using two identical sets of microscope lenses which are linked by an optical bridge.
ISBN:0-85404-539-2
Microscopy where the specimen is illuminated with visible light split into two beams, which then interfere to produce fringes whose spacing is proportional to the height of the specimen.
IOM
OIM
interference optical microscopy
CHMO:0000106
optical interference microscopy
Microscopy where the specimen is illuminated with visible light split into two beams, which then interfere to produce fringes whose spacing is proportional to the height of the specimen.
https://orcid.org/0000-0002-0640-0422
Microscopy where the specimen is illuminated with polarised visible light split into two beams, which then interfere to produce fringes whose spacing is proportional to the height of the specimen.
DIC
DIC microscopy
NIC
NIC microscopy
Nomarski interference contrast microscopy
Nomarski microscopy
CHMO:0000107
differential interference contrast microscopy
Microscopy where the specimen is illuminated with polarised visible light split into two beams, which then interfere to produce fringes whose spacing is proportional to the height of the specimen.
https://orcid.org/0000-0002-0640-0422
Microscopy where the specimen is illuminated with short-coherence length visible light split into two beams, which then interfere to produce fringes whose spacing is proportional to the height of the specimen.
CHMO:0000108
low coherence interference microscopy
Microscopy where the specimen is illuminated with short-coherence length visible light split into two beams, which then interfere to produce fringes whose spacing is proportional to the height of the specimen.
ISBN:0824742524
Microscopy where the surface of the specimen is illuminated with short-coherence length visible light split into two beams, which then interfere to produce fringes whose spacing is proportional to the profile of the specimen.
CPM
coherence-probe microscopy
phase correlation microscopy
CHMO:0000109
coherence probe microscopy
Microscopy where the surface of the specimen is illuminated with short-coherence length visible light split into two beams, which then interfere to produce fringes whose spacing is proportional to the profile of the specimen.
ISBN:0824742524
Microscopy where a transparent specimen is illuminated with visible light and small phase shifts in the light passing through the specimen are used to produce an image.
PCM
phase-contrast microscopy
CHMO:0000110
phase contrast microscopy
Microscopy where a transparent specimen is illuminated with visible light and small phase shifts in the light passing through the specimen are used to produce an image.
https://orcid.org/0000-0002-0640-0422
Microscopy where the specimen placed between two orthogonal polarising filters and illuminated with visible light.
PLM
POM
optical polarisation microscopy
optical polarising microscopy
optical polarization microscopy
polarised light microscopy
polarised optical microscopy
polarized light microscopy
polarized light optical microscopy
polarized optical microscopy
polarizing light microscopy
polarizing optical microscopy
CHMO:0000111
polarising light microscopy
Microscopy where the specimen placed between two orthogonal polarising filters and illuminated with visible light.
https://orcid.org/0000-0002-0640-0422
Microscopy which uses a probe to scan the surface of the specimen and measure some form of interaction between surface and probe. An image of the surface is obtained by mechanically moving the probe in a raster scan of the specimen, line by line, and recording the probe-surface interaction as a function of position. A feedback loop is used to maintain a fixed relationship between the probe and surface during scanning.
SPM
scanning-probe microscopy
CHMO:0000112
scanning probe microscopy
Microscopy which uses a probe to scan the surface of the specimen and measure some form of interaction between surface and probe. An image of the surface is obtained by mechanically moving the probe in a raster scan of the specimen, line by line, and recording the probe-surface interaction as a function of position. A feedback loop is used to maintain a fixed relationship between the probe and surface during scanning.
FIX:0000121
ISBN:1-86094-199-0
Microscopy which uses a sharp spike (known as a 'tip') mounted on the end of a cantilever to scan the surface of the specimen. An image of the surface is obtained by mechanically moving the probe in a raster scan of the specimen, line by line, and recording the force experienced by the tip as a function of position. A feedback loop is used to maintain a fixed relationship between the tip and surface during scanning.
AFM
SFM
atomic force imaging
atomic-force microscopy
scanning force microscopy
CHMO:0000113
atomic force microscopy
Microscopy which uses a sharp spike (known as a 'tip') mounted on the end of a cantilever to scan the surface of the specimen. An image of the surface is obtained by mechanically moving the probe in a raster scan of the specimen, line by line, and recording the force experienced by the tip as a function of position. A feedback loop is used to maintain a fixed relationship between the tip and surface during scanning.
FIX:0000114
https://orcid.org/0000-0002-0640-0422
Microscopy where an electric field is applied to a sharp spike (known as a 'tip') which is mounted on the end of a cantilever. The tip scans the surface of a piezoelectric specimen and the distortion of the electric field by the specimen is measured as a function of position. A feedback loop is used to maintain a fixed relationship between the tip and surface during scanning.
piezo-force microscopy
PFM
CHMO:0000114
piezoresponse force microscopy
Microscopy where an electric field is applied to a sharp spike (known as a 'tip') which is mounted on the end of a cantilever. The tip scans the surface of a piezoelectric specimen and the distortion of the electric field by the specimen is measured as a function of position. A feedback loop is used to maintain a fixed relationship between the tip and surface during scanning.
https://doi.org/10.1007/s10853-005-7244-2
PFM
Microscopy which uses a sharp magnetic spike (known as a 'tip') mounted on the end of a cantilever to scan the surface of a magnetic specimen. An image of the surface is obtained by mechanically moving the tip in a raster scan of the specimen, line by line, and recording the magnetic force experienced by it as a function of position. A feedback loop is used to maintain a fixed relationship between the tip and surface during scanning.
MFM
magnetic-force microscopy
CHMO:0000115
magnetic force microscopy
Microscopy which uses a sharp magnetic spike (known as a 'tip') mounted on the end of a cantilever to scan the surface of a magnetic specimen. An image of the surface is obtained by mechanically moving the tip in a raster scan of the specimen, line by line, and recording the magnetic force experienced by it as a function of position. A feedback loop is used to maintain a fixed relationship between the tip and surface during scanning.
FIX:0000118
ISBN:1-86094-199-0
Microscopy where optical tweezers are used to trap a small fluorescent latex bead which is then scanned across biological specimens in aqueous solution. An image of the surface is obtained by mechanically moving the bead in a raster scan of the specimen, line by line, and recording the fluorescence intensity as a function of position. A feedback loop is used to maintain a fixed relationship between the bead and surface during scanning.
PFM
photonic-force microscopy
CHMO:0000116
photonic force microscopy
Microscopy where optical tweezers are used to trap a small fluorescent latex bead which is then scanned across biological specimens in aqueous solution. An image of the surface is obtained by mechanically moving the bead in a raster scan of the specimen, line by line, and recording the fluorescence intensity as a function of position. A feedback loop is used to maintain a fixed relationship between the bead and surface during scanning.
https://doi.org/10.1006/jsbi.1997.3881
Microscopy which uses a small electrode to scan the surface of the specimen. An image of the surface is obtained by mechanically moving the probe in a raster scan of the specimen, line by line, and recording the electrostatic capacitance of the surface as a function of position. A feedback loop is used to maintain a fixed relationship between the electrode and surface during scanning.
SCAM
scanning-capacitance microscopy
CHMO:0000117
scanning capacitance microscopy
Microscopy which uses a small electrode to scan the surface of the specimen. An image of the surface is obtained by mechanically moving the probe in a raster scan of the specimen, line by line, and recording the electrostatic capacitance of the surface as a function of position. A feedback loop is used to maintain a fixed relationship between the electrode and surface during scanning.
https://orcid.org/0000-0002-0640-0422
Any type of microscopy where a probe is positioned very close to the surface of the specimen (in the near-field). An image of the surface is obtained by mechanically moving the probe in a raster scan of the specimen, line by line, and recording the probe-surface interaction as a function of position. A feedback loop is used to maintain a fixed relationship between the probe and surface during scanning.
near-field scanning microscopy
CHMO:0000118
scanning near-field microscopy
Any type of microscopy where a probe is positioned very close to the surface of the specimen (in the near-field). An image of the surface is obtained by mechanically moving the probe in a raster scan of the specimen, line by line, and recording the probe-surface interaction as a function of position. A feedback loop is used to maintain a fixed relationship between the probe and surface during scanning.
https://orcid.org/0000-0002-0640-0422
Microscopy where the specimen is illuminated with a near-field of photons. An image of the surface is obtained by mechanically moving an optical fibre probe in a raster scan over the specimen, line by line, and detecting any photons which tunnel from the specimen to the probe as a function of position. A feedback loop is used to maintain a fixed relationship between the optical fibre probe and surface during scanning.
PSTM
photon scanning tunneling microscopy
photon-scanning tunneling microscopy
photon-scanning tunnelling microscopy
CHMO:0000119
photon scanning tunnelling microscopy
Microscopy where the specimen is illuminated with a near-field of photons. An image of the surface is obtained by mechanically moving an optical fibre probe in a raster scan over the specimen, line by line, and detecting any photons which tunnel from the specimen to the probe as a function of position. A feedback loop is used to maintain a fixed relationship between the optical fibre probe and surface during scanning.
USPatent:5018865
Microscopy where a probe consisting of a laser transmitted through a tapered optical fibre is positioned very close to (<10 nm from) the surface of the specimen. The tip is coated with metal (to prevent light from escaping from the sides) and near-field (or evanescent field) light is emitted through a small opening or 'aperture' (50–100 nm in diameter) at the apex of the probe. An image is produced by scanning the probe over the specimen and detecting the disturbance of the near-field as a function of position. A force feedback loop is used to maintain a fixed relationship between the probe and surface during scanning.
NSOM
SNOM
aperture NSOM
aperture SNOM
aperture scanning near-field optical microscopy
aperture-NSOM
aperture-SNOM
near-field scanning optical microscopy
CHMO:0000120
scanning near-field optical microscopy
Microscopy where a probe consisting of a laser transmitted through a tapered optical fibre is positioned very close to (<10 nm from) the surface of the specimen. The tip is coated with metal (to prevent light from escaping from the sides) and near-field (or evanescent field) light is emitted through a small opening or 'aperture' (50–100 nm in diameter) at the apex of the probe. An image is produced by scanning the probe over the specimen and detecting the disturbance of the near-field as a function of position. A force feedback loop is used to maintain a fixed relationship between the probe and surface during scanning.
FIX:0000385
ISBN:1-86094-199-0
Microscopy where a probe consisting of a laser of a specific wavelength transmitted through a tapered optical fibre is positioned very close to (<10 nm from) the surface of the specimen. The tip is coated with metal (to prevent light from escaping from the sides) and near-field (or evanescent field) light is emitted through a small opening or 'aperture' (50–100 nm in diameter) at the apex of the probe. An image is produced by scanning the probe over the specimen and detecting the fluorescence intensity from fluorophores on the surface of the specimen as a function of position. A force feedback loop is used to maintain a fixed relationship between the probe and surface during scanning.
CHMO:0000121
fluorescence scanning near-field optical microscopy
Microscopy where a probe consisting of a laser of a specific wavelength transmitted through a tapered optical fibre is positioned very close to (<10 nm from) the surface of the specimen. The tip is coated with metal (to prevent light from escaping from the sides) and near-field (or evanescent field) light is emitted through a small opening or 'aperture' (50–100 nm in diameter) at the apex of the probe. An image is produced by scanning the probe over the specimen and detecting the fluorescence intensity from fluorophores on the surface of the specimen as a function of position. A force feedback loop is used to maintain a fixed relationship between the probe and surface during scanning.
https://orcid.org/0000-0002-0640-0422
Microscopy where a probe consisting of an infrared laser transmitted through a tapered optical fibre is positioned very close to (<10 nm from) the surface of the specimen. The tip is coated with metal (to prevent light from escaping from the sides) and near-field (or evanescent field) infrared radiation is emitted through a small opening or 'aperture' (50–100 nm in diameter) at the apex of the probe. An image is produced by scanning the probe over the specimen and detecting the disturbance of the infrared near-field as a function of position. A force feedback loop is used to maintain a fixed relationship between the probe and surface during scanning.
IR-NSOM
IR-SNOM
SNFIM
SNIM
SNIM imaging
infra-red near-field scanning optical microscopy
infra-red scanning near-field optical microscopy
infrared near-field scanning optical microscopy
CHMO:0000122
infrared scanning near-field optical microscopy
Microscopy where a probe consisting of an infrared laser transmitted through a tapered optical fibre is positioned very close to (<10 nm from) the surface of the specimen. The tip is coated with metal (to prevent light from escaping from the sides) and near-field (or evanescent field) infrared radiation is emitted through a small opening or 'aperture' (50–100 nm in diameter) at the apex of the probe. An image is produced by scanning the probe over the specimen and detecting the disturbance of the infrared near-field as a function of position. A force feedback loop is used to maintain a fixed relationship between the probe and surface during scanning.
https://doi.org/10.1016/j.jallcom.2005.02.057
Microscopy where a probe consisting of a microwave radiation source transmitted through a tapered optical fibre is positioned very close to (<10 nm from) the surface of the specimen. The tip is coated with metal (to prevent light from escaping from the sides) and near-field (or evanescent field) microwave radiation is emitted through a small opening or 'aperture' (50-100 nm in diameter) at the apex of the probe. An image is produced by scanning the probe over the specimen and detecting the disturbance of the microwave near-field as a function of position. A force feedback loop is used to maintain a fixed relationship between the probe and surface during scanning.
NSMM
SNMM
microwave near-field scanning microscopy
near-field scanning microwave microscopy
CHMO:0000123
microwave scanning near-field microscopy
Microscopy where a probe consisting of a microwave radiation source transmitted through a tapered optical fibre is positioned very close to (<10 nm from) the surface of the specimen. The tip is coated with metal (to prevent light from escaping from the sides) and near-field (or evanescent field) microwave radiation is emitted through a small opening or 'aperture' (50-100 nm in diameter) at the apex of the probe. An image is produced by scanning the probe over the specimen and detecting the disturbance of the microwave near-field as a function of position. A force feedback loop is used to maintain a fixed relationship between the probe and surface during scanning.
https://orcid.org/0000-0002-0640-0422
Microscopy where a laser spot is focused on a solid sharp metallic probe producing a confined light field very close to (<10 nm from) the surface of the specimen. An image is produced by scanning the probe over the specimen and detecting the scattering of the incident light by the probe as a function of position. A force feedback loop is used to maintain a fixed relationship between the probe and surface during scanning.
aNSOM
aSNOM
apertureless scanning near-field optical microscopy
scattering type apertureless near-field scanning optical microscopy
scattering type apertureless scanning near-field optical microscopy
scattering type near-field scanning optical microscopy
scattering type scanning near-field optical microscopy
CHMO:0000124
apertureless near-field scanning optical microscopy
Microscopy where a laser spot is focused on a solid sharp metallic probe producing a confined light field very close to (<10 nm from) the surface of the specimen. An image is produced by scanning the probe over the specimen and detecting the scattering of the incident light by the probe as a function of position. A force feedback loop is used to maintain a fixed relationship between the probe and surface during scanning.
https://doi.org/10.1039/b815925d
Microscopy where a laser spot is focused on a solid sharp noble metal probe very close to (<10 nm from) the surface of the specimen. The laser spot excites plasmons at the probe-surface interface and an image is produced by scanning the probe over the specimen and detecting the electromagnetic field as a function of position. A force feedback loop is used to maintain a fixed relationship between the probe and surface during scanning.
SPNM
scanning-plasmon near-field microscopy
CHMO:0000125
scanning plasmon near-field microscopy
Microscopy where a laser spot is focused on a solid sharp noble metal probe very close to (<10 nm from) the surface of the specimen. The laser spot excites plasmons at the probe-surface interface and an image is produced by scanning the probe over the specimen and detecting the electromagnetic field as a function of position. A force feedback loop is used to maintain a fixed relationship between the probe and surface during scanning.
https://doi.org/10.1039/b109955h
Microscopy where a thermocouple probe is positioned very close to the surface of the specimen (in the near-field). An image of the surface is obtained by mechanically moving the thermocouple probe in a raster scan of the specimen, line by line, and recording the surface–probe heat transfer as a function of position. A feedback loop is used to maintain a fixed relationship between the probe and surface during scanning.
NSThM
SNThM
near-field scanning thermal microscopy
CHMO:0000126
scanning near-field thermal microscopy
Microscopy where a thermocouple probe is positioned very close to the surface of the specimen (in the near-field). An image of the surface is obtained by mechanically moving the thermocouple probe in a raster scan of the specimen, line by line, and recording the surface–probe heat transfer as a function of position. A feedback loop is used to maintain a fixed relationship between the probe and surface during scanning.
https://orcid.org/0000-0002-0640-0422
Microscopy where an electrode probe is positioned very close to the surface of the specimen (in the near-field). The surface is mechanically scanned by the electrode in a raster scan and the height required by a feedback loop in order to maintain a constant electrical conductance between the electrode and the specimen is recorded as a function of position.
SECM
scanning-electrochemical microscopy
CHMO:0000127
scanning electrochemical microscopy
Microscopy where an electrode probe is positioned very close to the surface of the specimen (in the near-field). The surface is mechanically scanned by the electrode in a raster scan and the height required by a feedback loop in order to maintain a constant electrical conductance between the electrode and the specimen is recorded as a function of position.
ISBN:1-86094-199-0
Microscopy where a probe consisting of a glass nano- or micro- pipette filled with electrolyte is positioned very close to (in the near-field of) a specimen which is held in an oppositely charge electrolyte. An image of the surface is obtained by mechanically moving the pipette in a raster scan of the specimen, line by line, and recording the ion conductance as a function of position. A feedback loop is used to maintain a fixed relationship between the probe and surface during scanning.
SICM
scanning-ion conductance microscopy
CHMO:0000128
scanning ion conductance microscopy
Microscopy where a probe consisting of a glass nano- or micro- pipette filled with electrolyte is positioned very close to (in the near-field of) a specimen which is held in an oppositely charge electrolyte. An image of the surface is obtained by mechanically moving the pipette in a raster scan of the specimen, line by line, and recording the ion conductance as a function of position. A feedback loop is used to maintain a fixed relationship between the probe and surface during scanning.
ISBN:1-86094-199-0
Microscopy where a probe vibrating at its resonant frequency is scanned over the specimen. An image of the surface is obtained by mechanically moving the probe in a raster scan of the specimen, line by line, and recording the resonant frequency (or the amplitude of vibration) of the tip as a function of position. A feedback loop is used to maintain a fixed relationship between the probe and surface during scanning.
SPAM
scanning acoustic microscopy
SAM
CHMO:0000129
scanning probe acoustic microscopy
Microscopy where a probe vibrating at its resonant frequency is scanned over the specimen. An image of the surface is obtained by mechanically moving the probe in a raster scan of the specimen, line by line, and recording the resonant frequency (or the amplitude of vibration) of the tip as a function of position. A feedback loop is used to maintain a fixed relationship between the probe and surface during scanning.
https://doi.org/10.1007/s10853-005-7244-2
SAM
Microscopy where a probe vibrating at its resonant frequency is positioned very close to the surface of the specimen (in the near-field). An image of the surface is obtained by mechanically moving the probe in a raster scan of the specimen, line by line, and recording the resonant frequency (or amplitude of vibration) of the tip as a function of position. A feedback loop is used to maintain a fixed relationship between the probe and surface during scanning.
NSAM
SNAM
near-field scanning acoustic microscopy
CHMO:0000130
scanning near-field acoustic microscopy
Microscopy where a probe vibrating at its resonant frequency is positioned very close to the surface of the specimen (in the near-field). An image of the surface is obtained by mechanically moving the probe in a raster scan of the specimen, line by line, and recording the resonant frequency (or amplitude of vibration) of the tip as a function of position. A feedback loop is used to maintain a fixed relationship between the probe and surface during scanning.
https://doi.org/10.1007/BF00694423
Microscopy where an Wollaston wire probe is scanned over the surface of the specimen and the height required by a feedback loop in order to maintain a constant temperature between the probe and the specimen is recorded as a function of position.
SThM
scanning-thermal microscopy
CHMO:0000131
scanning thermal microscopy
Microscopy where an Wollaston wire probe is scanned over the surface of the specimen and the height required by a feedback loop in order to maintain a constant temperature between the probe and the specimen is recorded as a function of position.
ISBN:1-86094-199-0
Microscopy which uses a sharp conducting probe (or 'tip') held very close (1 nm) to the surface of the specimen. A bias voltage is applied between the tip and specimen which causes a tunnelling current to flow. An image is obtained by mechanically moving the probe in a raster scan of the specimen, line by line, and recording the tunnelling current as a function of position.
FIX:0000112
STM
scanning tunneling electron microscopy
scanning tunnelling electron microscopy
scanning-tunneling electron microscopy
scanning-tunnelling microscopy
CHMO:0000132
scanning tunnelling microscopy
Microscopy which uses a sharp conducting probe (or 'tip') held very close (1 nm) to the surface of the specimen. A bias voltage is applied between the tip and specimen which causes a tunnelling current to flow. An image is obtained by mechanically moving the probe in a raster scan of the specimen, line by line, and recording the tunnelling current as a function of position.
ISBN:1-86094-199-0
Microscopy where an excitation laser and a probe laser are focused onto a specimen forming a refractive index distribution which results in a concave excitation beam. The strength of this lens is proportional to the sample concentration and is detected by a change in transmittance in the probe beam.
TLM
thermal-lens microscopy
CHMO:0000133
thermal lens microscopy
Microscopy where an excitation laser and a probe laser are focused onto a specimen forming a refractive index distribution which results in a concave excitation beam. The strength of this lens is proportional to the sample concentration and is detected by a change in transmittance in the probe beam.
https://doi.org/10.1021/ac05196u
Thermal lens microscopy where the excitation laser is an ultraviolet laser.
UV-TLM
ultra-violet thermal-lens microscopy
ultraviolet thermal lens microscopy
ultraviolet thermal-lens microscopy
CHMO:0000134
ultra-violet thermal lens microscopy
Thermal lens microscopy where the excitation laser is an ultraviolet laser.
https://doi.org/10.1021/ac05196u
The measurement of the profile of a surface in order to quantify its roughness.
surface profilometry
SP
CHMO:0000135
profilometry
The measurement of the profile of a surface in order to quantify its roughness.
https://orcid.org/0000-0002-0640-0422
SP
A method where the profile of a surface is determined by moving a diamond stylus laterally across it at a specified contact force and measuring its vertical displacement.
CHMO:0000136
contact profilometry
A method where the profile of a surface is determined by moving a diamond stylus laterally across it at a specified contact force and measuring its vertical displacement.
https://orcid.org/0000-0002-0640-0422
A method where the profile of a surface is determined by illuminating the sample with a beam of light which has been split into two paths, one of which is directed at the sample and the other at a reference mirror. When the reflections are recombined any interference contains information about the contours of the surface.
non-contact profilometry
CHMO:0000137
optical profilometry
A method where the profile of a surface is determined by illuminating the sample with a beam of light which has been split into two paths, one of which is directed at the sample and the other at a reference mirror. When the reflections are recombined any interference contains information about the contours of the surface.
https://doi.org/10.1039/b807820c
A method where the profile of a surface is determined by illuminating the sample with a beam of light which has been split into two paths, one of which is directed at the sample and the other at a reference mirror. When the reflections are recombined a Fourier transform is applied to the phase of the interference pattern which contains information about the contours of the surface.
Fourier transform profilometry
FP
FTP
CHMO:0000138
Fourier profilometry
A method where the profile of a surface is determined by illuminating the sample with a beam of light which has been split into two paths, one of which is directed at the sample and the other at a reference mirror. When the reflections are recombined a Fourier transform is applied to the phase of the interference pattern which contains information about the contours of the surface.
ISBN:9051993080
FP
FTP
A method where the profile of a surface is determined by illuminating the sample with a beam of light which has been split into two paths, one of which is directed at the sample and the other at a reference mirror. When the reflections are recombined any distortions of periodic shadows due to interference contain information about the contours of the surface.
PP
CHMO:0000139
phase profilometry
A method where the profile of a surface is determined by illuminating the sample with a beam of light which has been split into two paths, one of which is directed at the sample and the other at a reference mirror. When the reflections are recombined any distortions of periodic shadows due to interference contain information about the contours of the surface.
https://doi.org/10.1061/40604(273)28
PP
Any detection or measurement method for a set of points in reciprocal space.
CHMO:0000140
reciprocal-space method
Any detection or measurement method for a set of points in reciprocal space.
https://orcid.org/0000-0002-0640-0422
Any detection or measurement method where the structure of a crystal or molecule can be determined by directing a beam of particles or radiation at a sample and recording the resulting diffraction pattern.
crystallography
diffraction analysis
CHMO:0000141
diffraction method
Any detection or measurement method where the structure of a crystal or molecule can be determined by directing a beam of particles or radiation at a sample and recording the resulting diffraction pattern.
FIX:0000004
FIX:0000217
https://orcid.org/0000-0002-0640-0422
A method for determining structure by directing a beam of electrons (the energies of which are controlled by their acceleration voltage) and recording the resulting diffraction pattern.
ED
electron crystallography
electron diffraction analysis
electron diffractometry
CHMO:0000142
electron diffraction
A method for determining structure by directing a beam of electrons (the energies of which are controlled by their acceleration voltage) and recording the resulting diffraction pattern.
FIX:0000009
ISBN:90190280031-0
A method for determining structure by directing a beam of electrons at the sample (the energies of which are controlled by their acceleration voltage) and recording the resulting diffraction pattern of any backscattered electrons.
BKD
EBSD
backscatter Kikuchi diffraction
CHMO:0000143
electron backscatter diffraction
A method for determining structure by directing a beam of electrons at the sample (the energies of which are controlled by their acceleration voltage) and recording the resulting diffraction pattern of any backscattered electrons.
https://orcid.org/0000-0002-0640-0422
A method for determining structure by directing a beam of high energy (10–200 keV) electrons at the sample and recording the resulting diffraction pattern.
HEED
high-energy electron diffraction
CHMO:0000144
high energy electron diffraction
A method for determining structure by directing a beam of high energy (10–200 keV) electrons at the sample and recording the resulting diffraction pattern.
Orange:17.3
A method for determining structure by directing a beam of high energy (10–200 keV) electrons at the sample and recording the resulting diffraction pattern produced by any electrons transmitted through the sample.
SADP
SAED
THEED
selected area electron diffraction
selected-area electron diffraction
transmission high-energy electron diffraction
CHMO:0000145
transmission high energy electron diffraction
A method for determining structure by directing a beam of high energy (10–200 keV) electrons at the sample and recording the resulting diffraction pattern produced by any electrons transmitted through the sample.
Orange:17.3
A method for determining structure by directing a beam of high energy (10–200 keV) electrons at the sample and recording the resulting diffraction pattern produced by any reflected or elastically scattered electrons.
RHEED
reflection high-energy electron diffraction
CHMO:0000146
reflection high energy electron diffraction
A method for determining structure by directing a beam of high energy (10–200 keV) electrons at the sample and recording the resulting diffraction pattern produced by any reflected or elastically scattered electrons.
https://doi.org/10.1351/goldbook.T06483
A method for determining structure by directing a beam of low energy (<500 eV) electrons at the sample and recording the resulting diffraction pattern.
LEED
CHMO:0000147
low energy electron diffraction
A method for determining structure by directing a beam of low energy (<500 eV) electrons at the sample and recording the resulting diffraction pattern.
ISBN:90190280031-0
Orange:17.3
A method for determining structure by directing a highly convergent beam (nm diameter) of low energy (<500 eV) electrons at the sample and recording the resulting diffraction pattern.
CBLEED
convergent beam low-energy electron diffraction
convergent-beam low-energy electron diffraction
CHMO:0000148
convergent beam low energy electron diffraction
A method for determining structure by directing a highly convergent beam (nm diameter) of low energy (<500 eV) electrons at the sample and recording the resulting diffraction pattern.
https://doi.org/10.1017/S1431927604040346
A method for determining structure by directing a beam of low energy (<500 eV) electrons at the sample and recording the resulting diffraction pattern produced by any elastically scattered (scattering where kinetic energy is conserved) electrons.
ELEED
elastic low-energy electron diffraction
low-energy electron diffraction
CHMO:0000149
elastic low energy electron diffraction
A method for determining structure by directing a beam of low energy (<500 eV) electrons at the sample and recording the resulting diffraction pattern produced by any elastically scattered (scattering where kinetic energy is conserved) electrons.
https://orcid.org/0000-0002-0640-0422
A method for determining structure by directing a beam of low energy (<500 eV) electrons at the sample and recording the resulting diffraction pattern produced by any inelastically scattered (scattering where kinetic energy is not conserved) electrons.
ILEED
inelastic low-energy electron diffraction
CHMO:0000150
inelastic low energy electron diffraction
A method for determining structure by directing a beam of low energy (<500 eV) electrons at the sample and recording the resulting diffraction pattern produced by any inelastically scattered (scattering where kinetic energy is not conserved) electrons.
https://orcid.org/0000-0002-0640-0422
A method for determining structure by directing a beam of high energy (<500 eV) electrons at the sample and recording the resulting diffraction pattern produced by any electrons transmitted through the sample.
TLEED
transmission low-energy electron diffraction
CHMO:0000151
transmission low energy electron diffraction
A method for determining structure by directing a beam of high energy (<500 eV) electrons at the sample and recording the resulting diffraction pattern produced by any electrons transmitted through the sample.
https://orcid.org/0000-0002-0640-0422
A method for determining structure during photoelectron spectroscopy. Photons are directed at the sample and diffraction patterns resulting from the emission of electrons are recorded.
PD
PED
PhD
CHMO:0000152
photoelectron diffraction
A method for determining structure during photoelectron spectroscopy. Photons are directed at the sample and diffraction patterns resulting from the emission of electrons are recorded.
Orange:17.2.1.6
PD
PhD
A method for determining structure during photoelectron spectroscopy. Photons are directed at a sample and diffraction patterns resulting from the emission of electrons are determined as a function of emission angle.
APD
APED
aziμthal-photoelectron diffraction
CHMO:0000153
aziμthal photoelectron diffraction
A method for determining structure during photoelectron spectroscopy. Photons are directed at a sample and diffraction patterns resulting from the emission of electrons are determined as a function of emission angle.
OrangeBook:17.2.1.6
A method for determining structure during photoelectron spectroscopy. Photons are directed at a sample and diffraction patterns resulting from the emission of electrons at 90° from the surface are recorded.
NPED
normal-photoelectron diffraction
NPD
CHMO:0000154
normal photoelectron diffraction
A method for determining structure during photoelectron spectroscopy. Photons are directed at a sample and diffraction patterns resulting from the emission of electrons at 90° from the surface are recorded.
Orange:17.2.1.6
NPD
A method for determining structure during X-ray photoelectron spectroscopy. X-rays are directed at a sample and diffraction patterns resulting from the emission of electrons are recorded.
XPD
XPED
XPhD
CHMO:0000155
X-ray photoelectron diffraction
A method for determining structure during X-ray photoelectron spectroscopy. X-rays are directed at a sample and diffraction patterns resulting from the emission of electrons are recorded.
Orange:17.2.1.6
A method for determining structure by directing a beam of X-rays at the sample and detecting the positions and intensities of the diffracted X-rays as a pattern of spots on a photographic plate.
X-Ray crystallographic analysis
X-ray analysis
X-ray crystallography
X-ray diffraction analysis
X-ray diffractometry
X-ray structure determination
XRD
CHMO:0000156
X-ray diffraction
A method for determining structure by directing a beam of X-rays at the sample and detecting the positions and intensities of the diffracted X-rays as a pattern of spots on a photographic plate.
FIX:0000007
ISBN:90190280031-0
A method for determining structure by detecting the positions and intensities of X-rays, that have been generated in microstructural domain, as a pattern of spots on a photographic plate.
Kossel technique
Kossel-technique
MXRD
micro X-ray diffraction
micro XRD
micro in situ XRD
CHMO:0000157
in situ micro-X-ray diffraction
A method for determining structure by detecting the positions and intensities of X-rays, that have been generated in microstructural domain, as a pattern of spots on a photographic plate.
Orange:17.3
A method for determining structure by directing a beam of X-rays at a powdered solid sample and detecting the positions and intensities of the diffracted X-rays as a pattern of spots on a photographic plate.
PXD
PXRD
X-ray powder diffraction
XRPD
powder XRD
CHMO:0000158
powder X-ray diffraction
A method for determining structure by directing a beam of X-rays at a powdered solid sample and detecting the positions and intensities of the diffracted X-rays as a pattern of spots on a photographic plate.
https://orcid.org/0000-0002-0640-0422
A method for determining structure by directing a beam of X-rays at a single crystal sample and detecting the positions and intensities of the diffracted X-rays as a pattern of spots on a photographic plate. Single crystal X-ray diffraction is used for protein crystallography.
single crystal X-ray crystallography
single-crystal X-ray diffraction
CHMO:0000159
single crystal X-ray diffraction
A method for determining structure by directing a beam of X-rays at a single crystal sample and detecting the positions and intensities of the diffracted X-rays as a pattern of spots on a photographic plate. Single crystal X-ray diffraction is used for protein crystallography.
https://orcid.org/0000-0002-0640-0422
Any detection or measurement method where reciprocal space structure can be determined by measuring the change in direction or energy of incident particles or radiation scattered by a sample.
CHMO:0000160
scattering method
Any detection or measurement method where reciprocal space structure can be determined by measuring the change in direction or energy of incident particles or radiation scattered by a sample.
https://doi.org/10.1351/goldbook.S05487
A method for determining structure by measuring the change in direction or energy of scattered alpha-particles.
alpha scattering
alpha-scattering
CHMO:0000161
alpha-particle scattering
A method for determining structure by measuring the change in direction or energy of scattered alpha-particles.
https://orcid.org/0000-0002-0640-0422
A method for determining structure by measuring the change in direction or energy of scattered atoms.
CHMO:0000162
atom scattering
A method for determining structure by measuring the change in direction or energy of scattered atoms.
OrangeBook:17.7.5
A method for determining structure by measuring the change in direction and energy of scattered He atoms. The He atoms suffer energy loss upon scattering by colliding inelastically with surfaces leading to the absorption or emission of surface phonons.
CHMO:0000163
inelastic atom scattering
A method for determining structure by measuring the change in direction and energy of scattered He atoms. The He atoms suffer energy loss upon scattering by colliding inelastically with surfaces leading to the absorption or emission of surface phonons.
https://orcid.org/0000-0002-0640-0422
Spectroscopy where a beam of electrons with a known, extended range of kinetic energies is scattered by a surface and the energy and position of the scattered electrons is measured.
ESS
electron scattering spectrometry
electron scattering spectroscopy
CHMO:0000164
electron scattering
Spectroscopy where a beam of electrons with a known, extended range of kinetic energies is scattered by a surface and the energy and position of the scattered electrons is measured.
FIX:0000401
FIX:0000666
OrangeBook:17.2.2.1
Spectroscopy where a beam of electrons with a known, extended range of kinetic energies is scattered by a sample supported on a nano-sized wire (such as a carbon nanotube) and the energy loss the electrons suffer upon scattering is measured.
NESS
nanowire electron scattering spectrometry
nanowire electron scattering spectroscopy
CHMO:0000165
nanowire electron scattering
Spectroscopy where a beam of electrons with a known, extended range of kinetic energies is scattered by a sample supported on a nano-sized wire (such as a carbon nanotube) and the energy loss the electrons suffer upon scattering is measured.
https://orcid.org/0000-0002-0640-0422
A method for determining structure by measuring the change in direction or energy of scattered visible light. Light is scattered by the electrons surrounding the atomic nuclei in the sample.
LS
LSS
LiSSP
light scattering spectrometry
light scattering spectroscopy
CHMO:0000166
light scattering
A method for determining structure by measuring the change in direction or energy of scattered visible light. Light is scattered by the electrons surrounding the atomic nuclei in the sample.
FIX:0000402
https://doi.org/10.1351/goldbook.L03525
LS
EXACT
A method for determining the size distribution of a sample of small particles in solution by illuminating the sample with a light source (usually a laser) and measuring the time-dependent fluctuations in the intensity of the scattered light caused by Brownian motion.
DLS
PCS
QELS
dynamic laser scattering
dynamic light scattering
dynamic light scattering spectrometry
dynamic light scattering spectroscopy
photocorrelation spectroscopy
photon correlation spectrometry
photon correlation spectroscopy
quasi-elastic light scattering
quasi-elastic light scattering spectrometry
quasi-elastic light scattering spectroscopy
CHMO:0000167
dynamic light scattering
A method for determining the size distribution of a sample of small particles in solution by illuminating the sample with a light source (usually a laser) and measuring the time-dependent fluctuations in the intensity of the scattered light caused by Brownian motion.
ISBN:0471705160
A method for determining structure by measuring the change in direction or energy of scattered visible light at a number of different angles, none of which are close to the angle of incidence of the light.
MALLS
MALS
multi angle light scattering
multi-angle laser light scattering
multi-angle light scattering spectrometry
multi-angle light scattering spectroscopy
multiangle light scattering
multiple angle laser light scattering
multiple angle laser light scattering spectrometry
multiple angle laser light scattering spectroscopy
multiple angle light scattering
multiple angle light scattering spectroscopy
multiple light scattering spectrometry
CHMO:0000168
multi-angle light scattering
A method for determining structure by measuring the change in direction or energy of scattered visible light at a number of different angles, none of which are close to the angle of incidence of the light.
https://orcid.org/0000-0002-0640-0422
A method for determining structure by measuring the change in direction or energy of Rayleigh scattered visible light.
Rayleigh scattering method
elastic light scattering
laser Rayleigh scattering
laser Rayleigh scattering spectrometry
laser Rayleigh scattering spectroscopy
laser-Rayleigh scattering
CHMO:0000169
Rayleigh scattering spectroscopy
A method for determining structure by measuring the change in direction or energy of Rayleigh scattered visible light.
FIX:0000059
https://doi.org/10.1007/978-3-540-72865-8
A method for determining structure by measuring the change in direction or energy of Rayleigh scattered visible light which has been passed through an inferometer.
interferometric Rayleigh scattering
interferometric Rayleigh scattering method
interferometric Rayleigh scattering spectrometry
CHMO:0000170
interferometric Rayleigh scattering spectroscopy
A method for determining structure by measuring the change in direction or energy of Rayleigh scattered visible light which has been passed through an inferometer.
https://orcid.org/0000-0002-0640-0422
A method for determining the structure of a liquid sample by measuring the change in direction or energy of hyper-Rayleigh scattered visible light (scattering where photons from the incident laser–-with frequency –-are scattered into photons of the second harmonic–-photons with frequency 2).
HRLS
SHLS
hyper Rayleigh light scattering
hyper Rayleigh scattering
hyper Rayleigh scattering spectrometry
hyper-Rayleigh light scattering
hyper-Rayleigh scattering
hyper-Rayleigh scattering spectrometry
hyper-Rayleigh scattering spectroscopy
second harmonic Rayleigh scattering
HRS
CHMO:0000171
hyper Rayleigh scattering spectroscopy
A method for determining the structure of a liquid sample by measuring the change in direction or energy of hyper-Rayleigh scattered visible light (scattering where photons from the incident laser–-with frequency –-are scattered into photons of the second harmonic–-photons with frequency 2).
ISBN:0849389097
HRS
A method for determining structure by measuring the change in direction or energy of Rayleigh scattered visible light, where the wavelength of the incident light does not correspond to any absorption bands in the scattering molecules.
non-resonance Rayleigh scattering
non-resonance Rayleigh scattering spectrometry
non-resonant Rayleigh scattering
off-resonance Rayleigh scattering
CHMO:0000172
non-resonance Rayleigh scattering spectroscopy
A method for determining structure by measuring the change in direction or energy of Rayleigh scattered visible light, where the wavelength of the incident light does not correspond to any absorption bands in the scattering molecules.
https://orcid.org/0000-0002-0640-0422
A method for determining structure by measuring the change in direction or energy of Rayleigh scattered visible light, where the wavelength of the incident light corresponds to an energy which is near to an absorption band in the scattering molecules.
NRRLS
NRRS
near-Rayleigh resonance scattering
near-Rayleigh resonant scattering
near-resonance Rayleigh light scattering
near-resonance Rayleigh scattering
near-resonance Rayleigh scattering spectrometry
near-resonant Rayleigh light scattering
near-resonant Rayleigh scattering
CHMO:0000173
near-resonance Rayleigh scattering spectroscopy
A method for determining structure by measuring the change in direction or energy of Rayleigh scattered visible light, where the wavelength of the incident light corresponds to an energy which is near to an absorption band in the scattering molecules.
https://orcid.org/0000-0002-0640-0422
A method for determining structure by measuring the change in direction or energy of Rayleigh scattered visible light, where the wavelength of the incident light corresponds to an absorption band in the scattering molecules.
RRLS
RRS
RRS detection
RRSD
resonance Rayleigh light scattering
resonance Rayleigh scattering
resonance Rayleigh scattering spectrometry
CHMO:0000174
resonance Rayleigh scattering spectroscopy
A method for determining structure by measuring the change in direction or energy of Rayleigh scattered visible light, where the wavelength of the incident light corresponds to an absorption band in the scattering molecules.
https://doi.org/10.1039/b101827m
A method for determining structure by measuring the change in direction or energy of Rayleigh scattered visible light, as a function of time, where the wavelength of the incident light corresponds to an absorption band in the scattering molecules.
time resolved resonance Rayleigh scattering spectrometry
time resolved resonance Rayleigh spectroscopy
time resolved resonant Rayleigh scattering spectrometry
time resolved resonant Rayleigh spectroscopy
time-resolved resonant Rayleigh scattering
time-resolved resonant Rayleigh scattering spectroscopy
CHMO:0000175
time-resolved resonance Rayleigh scattering
A method for determining structure by measuring the change in direction or energy of Rayleigh scattered visible light, as a function of time, where the wavelength of the incident light corresponds to an absorption band in the scattering molecules.
https://orcid.org/0000-0002-0640-0422
A method for determining structure where a grating created by the interference of two laser beams is written into a sample and a further laser beam is Rayleigh scattered by the grating. The change in direction or energy of the light and the temporal evolution of the scattered beam are measured.
FRLS
FRS
forced Rayleigh light scattering
forced Rayleigh light scattering spectrometry
forced Rayleigh light scattering spectroscopy
forced Rayleigh scattering
forced Rayleigh scattering spectrometry
CHMO:0000176
forced Rayleigh scattering spectroscopy
A method for determining structure where a grating created by the interference of two laser beams is written into a sample and a further laser beam is Rayleigh scattered by the grating. The change in direction or energy of the light and the temporal evolution of the scattered beam are measured.
https://doi.org/10.1007/BF00694201
A method for determining structure where a grating created by the interference of two laser beams is written into a sample which contains a small amount of dye. The intensity grating is converted into a temperature grating which, in turn, causes a concentration grating by thermal diffusion. A further laser beam is Rayleigh scattered by the grating and the change in direction or energy of the light and the temporal evolution of the scattered beam are measured.
S-FRS
S-FRSM
SFRS
SFRSM
Soret forced Rayleigh scattering method
TDFRS
TDFRS analysis
TDFRS method
thermal diffusion forced Rayleigh scattering
thermal-diffusion forced Rayleigh scattering
CHMO:0000177
thermal diffusion forced Rayleigh scattering
A method for determining structure where a grating created by the interference of two laser beams is written into a sample which contains a small amount of dye. The intensity grating is converted into a temperature grating which, in turn, causes a concentration grating by thermal diffusion. A further laser beam is Rayleigh scattered by the grating and the change in direction or energy of the light and the temporal evolution of the scattered beam are measured.
https://doi.org/10.1039/b810860a
A method for determining structure where a grating created by the interference of infrared laser beams is written into a sample which contains a small amount of dye. The intensity grating is converted into a temperature grating which, in turn, causes a concentration grating by thermal diffusion. A further infrared laser beam is Rayleigh scattered by the grating and the change in direction or energy of the light and the temporal evolution of the scattered beam are measured.
IR-TDFRS
IR-TDFRS analysis
IR-TDFRS method
infrared thermal diffusion forced Rayleigh scattering
CHMO:0000178
infrared thermal diffusion forced Rayleigh scattering
A method for determining structure where a grating created by the interference of infrared laser beams is written into a sample which contains a small amount of dye. The intensity grating is converted into a temperature grating which, in turn, causes a concentration grating by thermal diffusion. A further infrared laser beam is Rayleigh scattered by the grating and the change in direction or energy of the light and the temporal evolution of the scattered beam are measured.
https://doi.org/10.1039/b810860a
A method for determining structure by measuring the change in direction or energy of visible light scattered at a small angle (0.1–10°) to the incident light.
LALLS
LALLSS
LALS
LALSS
SALS
SALSS
low angle laser light scattering
low angle laser light scattering spectroscopy
low angle light scattering
low angle light scattering spectrometry
low angle light scattering spectroscopy
small angle light scattering
CHMO:0000179
small-angle light scattering
A method for determining structure by measuring the change in direction or energy of visible light scattered at a small angle (0.1–10°) to the incident light.
FIX:0000254
https://orcid.org/0000-0002-0640-0422
A method for determining structure by measuring the total or time-averaged scattering intensity of scattered visible light as a function of angle.
DLSS
TILS
classical light scattering
differential light scattering
differential light-scattering spectroscopy
differential static light scattering
integrated light scattering
static light scattering
static light scattering spectrometry
static light scattering spectroscopy
total intensity light scattering
traditional light scattering
SLS
CHMO:0000180
static light scattering
A method for determining structure by measuring the total or time-averaged scattering intensity of scattered visible light as a function of angle.
https://orcid.org/0000-0002-0640-0422
A method for determining structure by measuring the change in direction or energy of scattered neutrons. Neutrons are scattered by the atomic nuclei in the sample and the intensity of the scattering is given by the scattering vector Q = (4/)sin(pi/2).
FIX:0000400
neutron scattering spectrometry
neutron scattering spectroscopy
CHMO:0000181
neutron scattering
A method for determining structure by measuring the change in direction or energy of scattered neutrons. Neutrons are scattered by the atomic nuclei in the sample and the intensity of the scattering is given by the scattering vector Q = (4/)sin(pi/2).
ISBN:0824719948
A method for determining structure by measuring the change in direction or energy of scattered neutrons. Neutrons are scattered by the atomic nuclei in the sample and phase is conserved.
CHMO:0000182
coherent neutron scattering
A method for determining structure by measuring the change in direction or energy of scattered neutrons. Neutrons are scattered by the atomic nuclei in the sample and phase is conserved.
https://orcid.org/0000-0002-0640-0422
A method for determining structure by measuring the change in direction of scattered neutrons. Neutrons are scattered by the atomic nuclei in the sample and retain all of their kinetic energy during collisions.
elastic neutron scattering
CHMO:0000183
elastic neutron scattering
A method for determining structure by measuring the change in direction of scattered neutrons. Neutrons are scattered by the atomic nuclei in the sample and retain all of their kinetic energy during collisions.
https://orcid.org/0000-0002-0640-0422
A method for determining structure by measuring the change in direction or energy of scattered neutrons at small angles (corresponding to a scattering vector Q = (4/)sin(\pi/2) = 0.005–0.2 inverse degrees).
FIX:0000253
SANS
low-Q neutron scattering
small angle neutron scattering
CHMO:0000184
small-angle neutron scattering
A method for determining structure by measuring the change in direction or energy of scattered neutrons at small angles (corresponding to a scattering vector Q = (4/)sin(\pi/2) = 0.005–0.2 inverse degrees).
ISBN:9056993003
A method for determining structure by measuring the change in direction or energy of neutrons scattered at low angles. The incident neutron beam strikes the sample under a small angle close to the critical angle of total external neutron reflection.
GISANS
CHMO:0000185
grazing incidence small-angle neutron scattering
A method for determining structure by measuring the change in direction or energy of neutrons scattered at low angles. The incident neutron beam strikes the sample under a small angle close to the critical angle of total external neutron reflection.
https://orcid.org/0000-0002-0640-0422
A method for determining structure by measuring the change in direction or energy of scattered neutrons at ultra-small angles (corresponding to Q = 0.000003–0.01 inverse degrees).
USANS
ultra-high resolution small-angle neutron scattering
CHMO:0000186
ultra small angle neutron scattering
A method for determining structure by measuring the change in direction or energy of scattered neutrons at ultra-small angles (corresponding to Q = 0.000003–0.01 inverse degrees).
https://orcid.org/0000-0002-0640-0422
A method for determining structure by measuring the change in direction or energy of scattered neutrons at wide angles (corresponding to Q >1 inverse degrees).
WANS
wide angle neutron scattering
CHMO:0000187
wide angle neutron scattering
A method for determining structure by measuring the change in direction or energy of scattered neutrons at wide angles (corresponding to Q >1 inverse degrees).
FIX:0001130
https://doi.org/10.1002/pol.1982.180200207
A method for determining structure by measuring the change in direction or energy of scattered neutrons. Neutrons are scattered by the atomic nuclei in the sample and phase is not conserved.
INS
CHMO:0000188
incoherent neutron scattering
A method for determining structure by measuring the change in direction or energy of scattered neutrons. Neutrons are scattered by the atomic nuclei in the sample and phase is not conserved.
https://doi.org/10.1039/b811090e
INS
A method for determining structure by measuring the change in direction of scattered neutrons. Neutrons are scattered by the atomic nuclei in the sample, phase is not conserved and the neutrons retain all of their kinetic energy during collisions.
EINS
CHMO:0000189
elastic incoherent neutron scattering
A method for determining structure by measuring the change in direction of scattered neutrons. Neutrons are scattered by the atomic nuclei in the sample, phase is not conserved and the neutrons retain all of their kinetic energy during collisions.
https://orcid.org/0000-0002-0640-0422
A method for determining structure by measuring the change in direction or energy of scattered neutrons. Neutrons are scattered by the atomic nuclei in a liquid sample which is in thermal motion. Phase is not conserved and although the neutrons retain all of their kinetic energy during collisions, the thermal motion of the sample causes a broadening of the energy range of the scattered neutrons.
QENS
QINS
quasi elastic neutron scattering
quasi elastic neutron scattering spectrometry
quasi elastic neutron scattering spectroscopy
quasi-elastic neutron scattering spectrometry
quasi-elastic neutron scattering spectroscopy
CHMO:0000190
quasi-elastic neutron scattering
A method for determining structure by measuring the change in direction or energy of scattered neutrons. Neutrons are scattered by the atomic nuclei in a liquid sample which is in thermal motion. Phase is not conserved and although the neutrons retain all of their kinetic energy during collisions, the thermal motion of the sample causes a broadening of the energy range of the scattered neutrons.
ISBN:082475056X
A method for determining structure by measuring the change in direction or energy of scattered neutrons. Neutrons are scattered by the atomic nuclei in the sample, phase is not conserved and the neutrons suffer a loss of kinetic energy during collisions.
IINS
incoherent inelastic neutron scattering
CHMO:0000191
inelastic incoherent neutron scattering
A method for determining structure by measuring the change in direction or energy of scattered neutrons. Neutrons are scattered by the atomic nuclei in the sample, phase is not conserved and the neutrons suffer a loss of kinetic energy during collisions.
https://orcid.org/0000-0002-0640-0422
A method for determining structure by measuring the change in direction or energy of scattered neutrons. Neutrons are scattered by the atomic nuclei in the sample, and suffer a loss of kinetic energy during collisions.
inelastic coherent neutron scattering
inelastic neutron scattering spectrometry
inelastic neutron scattering spectroscopy
INS
CHMO:0000192
inelastic neutron scattering
A method for determining structure by measuring the change in direction or energy of scattered neutrons. Neutrons are scattered by the atomic nuclei in the sample, and suffer a loss of kinetic energy during collisions.
Orange:17.7.5
A method for determining structure by measuring the change in direction or energy of backscattered neutrons. Neutrons are scattered by the atomic nuclei in the sample, and suffer a loss of kinetic energy during collisions.
neutron backscattering
neutron backscattering spectrometry
neutron backscattering spectroscopy
CHMO:0000193
neutron backscattering
A method for determining structure by measuring the change in direction or energy of backscattered neutrons. Neutrons are scattered by the atomic nuclei in the sample, and suffer a loss of kinetic energy during collisions.
https://orcid.org/0000-0002-0640-0422
A method for determining structure by measuring the change in direction or energy of scattered neutrons and the time since the indicent pulse ('time-of-flight') for each neutron. Neutrons are scattered by the atomic nuclei in the sample, and suffer a loss of kinetic energy during collisions.
CHMO:0000194
neutron time-of-flight scattering
A method for determining structure by measuring the change in direction or energy of scattered neutrons and the time since the indicent pulse ('time-of-flight') for each neutron. Neutrons are scattered by the atomic nuclei in the sample, and suffer a loss of kinetic energy during collisions.
https://orcid.org/0000-0002-0640-0422
A method for determining structure by measuring the change in direction, energy and momentum of scattered neutrons. Neutrons are scattered by the atomic nuclei in the sample, and suffer a loss of kinetic energy during collisions.
TAS
triple-axis neutron scattering
triple-axis neutron scattering spectrometry
triple-axis neutron spectrometry
triple-axis neutron spectroscopy
CHMO:0000195
triple-axis neutron scattering
A method for determining structure by measuring the change in direction, energy and momentum of scattered neutrons. Neutrons are scattered by the atomic nuclei in the sample, and suffer a loss of kinetic energy during collisions.
https://orcid.org/0000-0002-0640-0422
A method for determining structure by measuring the velocity of neutrons in known magnetic fields before and after scattering by the sample. The neutrons are scattered by the interaction of neutron spin with spins in the sample ('spin echo').
neutron spin echo spectrometry
neutron spin echo spectroscopy
neutron spin-echo spectrometry
neutron spin-echo spectroscopy
spin-echo neutrons scattering
CHMO:0000196
spin-echo neutron scattering
A method for determining structure by measuring the velocity of neutrons in known magnetic fields before and after scattering by the sample. The neutrons are scattered by the interaction of neutron spin with spins in the sample ('spin echo').
https://orcid.org/0000-0002-0640-0422
A method for determining structure by measuring the velocity of neutrons in known magnetic fields before and after scattering at small angles by the sample. The neutrons are scattered by the interaction of neutron spin with spins in the sample ('spin echo').
SEANS
non-magnetic SEANS
non-magnetic spin-echo SANS
non-magnetic spin-echo small angle neutron scattering
spin-echo SANS
spin-echo small angle neutron scattering
CHMO:0000197
spin-echo small angle neutron scattering
A method for determining structure by measuring the velocity of neutrons in known magnetic fields before and after scattering at small angles by the sample. The neutrons are scattered by the interaction of neutron spin with spins in the sample ('spin echo').
https://doi.org/10.1107/S0021889808026770
A method for determining structure by measuring the velocity of neutrons in known magnetic fields before and after scattering at small angles by a magnetic sample. The neutrons are scattered by the interaction of neutron spin with spins in the sample ('spin echo').
magnetic SEANS
CHMO:0000198
magnetic spin-echo small angle neutron scattering
A method for determining structure by measuring the velocity of neutrons in known magnetic fields before and after scattering at small angles by a magnetic sample. The neutrons are scattered by the interaction of neutron spin with spins in the sample ('spin echo').
https://orcid.org/0000-0002-0640-0422
A method for determining structure by measuring the velocity of neutrons in known magnetic fields before and after scattering at wide angles by the sample. The neutrons are scattered by the interaction of neutron spin with spins in the sample ('spin echo').
CHMO:0000199
spin-echo wide angle neutron scattering
A method for determining structure by measuring the velocity of neutrons in known magnetic fields before and after scattering at wide angles by the sample. The neutrons are scattered by the interaction of neutron spin with spins in the sample ('spin echo').
https://orcid.org/0000-0002-0640-0422
A method for determining structure by measuring the change in direction or energy of X-rays scattered by a sample.
XRS
XS
CHMO:0000200
X-ray scattering
A method for determining structure by measuring the change in direction or energy of X-rays scattered by a sample.
FIX:0000073
https://orcid.org/0000-0002-0640-0422
A method for determining structure by measuring the energy loss of X-rays scattered by a sample.
IXS
IXSS
X-ray Raman spectrometry
X-ray Raman spectroscopy
XSS
inelastic X-ray scattering
inelastic X-ray scattering spectrometry
inelastic X-ray scattering spectroscopy
non-resonant inelastic X-ray emission spectrometry
non-resonant inelastic X-ray emission spectroscopy
non-resonant inelastic X-ray scattering
CHMO:0000201
inelastic X-ray scattering
A method for determining structure by measuring the energy loss of X-rays scattered by a sample.
https://orcid.org/0000-0002-0640-0422
A method for determining structure by measuring the energy loss of X-rays scattered by a sample where the incident X-ray energy is chosen to coincide with an electronic transition in the sample.
RIXES
RIXS
resonant inelastic X-ray emission spectrometry
resonant inelastic X-ray emission spectroscopy
resonant inelastic X-ray scattering spectrometry
resonant inelastic X-ray scattering spectroscopy
CHMO:0000202
resonant inelastic X-ray scattering
A method for determining structure by measuring the energy loss of X-rays scattered by a sample where the incident X-ray energy is chosen to coincide with an electronic transition in the sample.
https://orcid.org/0000-0002-0640-0422
A method for determining structure by measuring the energy loss of X-rays scattered by a sample as a function of emission angle, where the incident X-ray energy is chosen to coincide with an electronic transition in the sample.
angle-resolved resonant X-ray emission spectrometry
angle-resolved resonant X-ray emission spectroscopy
angular-resolved resonant X-ray emission spectroscopy
CHMO:0000203
angle-resolved resonant X-ray scattering
A method for determining structure by measuring the energy loss of X-rays scattered by a sample as a function of emission angle, where the incident X-ray energy is chosen to coincide with an electronic transition in the sample.
https://orcid.org/0000-0002-0640-0422
A method for determining structure by measuring the change in direction or energy of X-rays scattered by a sample at low angles (0–10°).
SAXS
small angle X-ray scattering
CHMO:0000204
small-angle X-ray scattering
A method for determining structure by measuring the change in direction or energy of X-rays scattered by a sample at low angles (0–10°).
FIX:0000223
https://orcid.org/0000-0002-0640-0422
A method for determining structure by measuring the change in direction or energy of X-rays scattered by a sample. The incident X-ray beam strikes the sample under a small angle close to the critical angle of total external X-ray reflection.
GISAXS
GIXS
grazing incidence X-ray scattering
grazing incidence small-angle X-ray scattering
grazing-incidence small-angle X-ray scattering
CHMO:0000205
grazing-incidence X-ray scattering
A method for determining structure by measuring the change in direction or energy of X-rays scattered by a sample. The incident X-ray beam strikes the sample under a small angle close to the critical angle of total external X-ray reflection.
https://orcid.org/0000-0002-0640-0422
A method for determining structure by measuring the change in direction or energy of X-rays scattered by a sample at ultra-low angles (corresponding to Q = 0.00005–0.005 inverse°).
USAXS
ultra small angle X-ray scattering
ultra small-angle X-ray scattering
ultra-small-angle X-ray scattering
CHMO:0000206
ultra-small angle X-ray scattering
A method for determining structure by measuring the change in direction or energy of X-rays scattered by a sample at ultra-low angles (corresponding to Q = 0.00005–0.005 inverse°).
https://doi.org/10.1021/la9803171
A method for determining structure by measuring the change in direction or energy of X-rays scattered by a sample at wide angles (>10°). Wide-angle X-ray scattering is used for determining the structure of polymers.
WAXS
wide angle X-ray scattering
CHMO:0000207
wide-angle X-ray scattering
A method for determining structure by measuring the change in direction or energy of X-rays scattered by a sample at wide angles (>10°). Wide-angle X-ray scattering is used for determining the structure of polymers.
FIX:0001128
https://orcid.org/0000-0002-0640-0422
Any method for determining structure where the change in direction or intensity of reflected radiation or particles is detected.
CHMO:0000208
reflection method
Any method for determining structure where the change in direction or intensity of reflected radiation or particles is detected.
https://orcid.org/0000-0002-0640-0422
Any method for determining structure by directing a beam of particles or X-rays onto an extremely flat surface and measuring the intensity of the reflected radiation as a function of angle.
reflectivity
CHMO:0000209
reflectometry
Any method for determining structure by directing a beam of particles or X-rays onto an extremely flat surface and measuring the intensity of the reflected radiation as a function of angle.
https://orcid.org/0000-0002-0640-0422
A method for determining structure by directing a beam of neutrons onto an extremely flat surface and measuring the intensity of the reflected neutrons as a function of angle and neutron wavelength.
neutron reflection
neutron reflectivity
specular neutron reflectivity
specular neutron reflectrometry
CHMO:0000210
neutron reflectometry
A method for determining structure by directing a beam of neutrons onto an extremely flat surface and measuring the intensity of the reflected neutrons as a function of angle and neutron wavelength.
https://orcid.org/0000-0002-0640-0422
A method for determining structure by illuminating an extremely flat surface with visible light and measuring the intensity of the reflected light as a function of angle. The reflected light has two polarised components, s (perpendicular) and p (parallel). The reflectivity of s-polarised light depends on the angle of incidence, but the reflectivity of p-polarised light vanishes at the Brewster angle.
OR
light laser reflectivity
light laser reflectometry
light reflectivity
light reflectometry
optical laser reflectivity
optical reflectivity
CHMO:0000211
optical reflectometry
A method for determining structure by illuminating an extremely flat surface with visible light and measuring the intensity of the reflected light as a function of angle. The reflected light has two polarised components, s (perpendicular) and p (parallel). The reflectivity of s-polarised light depends on the angle of incidence, but the reflectivity of p-polarised light vanishes at the Brewster angle.
https://doi.org/10.1039/b716178f
A method for determining structure by illuminating an extremely flat surface with visible light and measuring the intensity of the light reflected at the Brewster angle.
fixed angle reflectivity
fixed-angle reflectivity
fixed-angle reflectometry
optical fixed angle reflectivity
optical fixed angle reflectometry
optical fixed-angle reflectivity
optical fixed-angle reflectometry
CHMO:0000212
fixed angle reflectometry
A method for determining structure by illuminating an extremely flat surface with visible light and measuring the intensity of the light reflected at the Brewster angle.
ISBN:0824700007
A method for determining structure by illuminating an extremely flat surface with visible light and interfering the light reflected from the sample at the Brewster angle with light reflected from a reference mirror. Intereference only occurs when the difference in the optical path lengths between the two mirrors is within the coherence length of the optical source.
OCDR
OLCR
optical coherence-domain reflectivity
optical low-coherence domain reflectivity
optical low-coherence domain reflectometry
CHMO:0000213
optical coherence-domain reflectometry
A method for determining structure by illuminating an extremely flat surface with visible light and interfering the light reflected from the sample at the Brewster angle with light reflected from a reference mirror. Intereference only occurs when the difference in the optical path lengths between the two mirrors is within the coherence length of the optical source.
ISBN:089603-574-3
A method for determining structure by illuminating an extremely flat surface with light from a pulsed laser and interfering the light reflected from the sample at the Brewster angle with light reflected from a reference mirror. Intereference only occurs when the difference in the optical path lengths between the two mirrors is within the coherence length of the optical source. The frequency of the laser pulse is proportional to the time delay between each of the signals returning.
OFDR
optical frequency domain reflectivity
optical frequency domain reflectometry
optical frequency-domain reflectivity
CHMO:0000214
optical frequency-domain reflectometry
A method for determining structure by illuminating an extremely flat surface with light from a pulsed laser and interfering the light reflected from the sample at the Brewster angle with light reflected from a reference mirror. Intereference only occurs when the difference in the optical path lengths between the two mirrors is within the coherence length of the optical source. The frequency of the laser pulse is proportional to the time delay between each of the signals returning.
ISBN:3540231048
A method for determining structure by directing an optical pulse through an optical fibre and measuring the intensity of light reflected at the Brewster angle as a function of time.
OTDR
optical time domain reflectivity
optical time domain reflectometry
optical time-domain reflectivity
optical time-domain reflectometry
CHMO:0000215
optical time-domain reflectometry
A method for determining structure by directing an optical pulse through an optical fibre and measuring the intensity of light reflected at the Brewster angle as a function of time.
ISBN:0471820539
A method for determining structure by directing an optical pulse through an optical fibre and measuring the polarisation state of light reflected at the Brewster angle as a function of time.
PODTR
polarisation OTDR
polarisation optical time domain reflectivity
polarisation optical time domain reflectometry
polarisation optical time-domain reflectivity
polarization OTDR
polarization optical time domain reflectivity
polarization optical time domain reflectometry
polarization optical time-domain reflectivity
CHMO:0000216
polarisation optical time-domain reflectometry
A method for determining structure by directing an optical pulse through an optical fibre and measuring the polarisation state of light reflected at the Brewster angle as a function of time.
ISBN:0471820539
A method for determining structure by illuminating an extremely flat surface with visible light and monitoring the intensity of light reflected at the Brewster angle during the adsorption of particles on the surface.
SPAR
stagnation point adsorption reflectivity
CHMO:0000217
stagnation point adsorption reflectometry
A method for determining structure by illuminating an extremely flat surface with visible light and monitoring the intensity of light reflected at the Brewster angle during the adsorption of particles on the surface.
https://doi.org/10.1039/b716178f
A method for determining structure by illuminating an extremely flat surface with visible light and measuring the intensity of light reflected at different angles around the Brewster angle.
scanning angle reflectivity
scanning-angle reflectivity
scanning-angle reflectometry
CHMO:0000218
scanning angle reflectometry
A method for determining structure by illuminating an extremely flat surface with visible light and measuring the intensity of light reflected at different angles around the Brewster angle.
ISBN:0824700007
A method for determining structure by directing a beam of X-rays at an extremely flat surface and measuring the intensity of the reflected X-rays as a function of angle. X-ray reflectometry is used to determine the structure of thin films.
X-ray reflectivity
XRR
CHMO:0000219
X-ray reflectometry
A method for determining structure by directing a beam of X-rays at an extremely flat surface and measuring the intensity of the reflected X-rays as a function of angle. X-ray reflectometry is used to determine the structure of thin films.
https://orcid.org/0000-0002-0640-0422
A method for determining structure by directing a beam of X-rays at an extremely flat surface (at angle theta minus omega to the surface) and measuring the intensity of the X-rays which undergo diffuse reflection (and are emitted at angle theta plus omega from the surface).
diffuse X-ray reflectance
diffuse XRR
off-specular X-ray reflectivity
off-specular X-ray reflectometry
off-specular XRR
CHMO:0000220
diffuse X-ray reflectometry
A method for determining structure by directing a beam of X-rays at an extremely flat surface (at angle theta minus omega to the surface) and measuring the intensity of the X-rays which undergo diffuse reflection (and are emitted at angle theta plus omega from the surface).
https://orcid.org/0000-0002-0640-0422
A method for determining structure by directing a beam of X-rays at an extremely flat surface (at a grazing angle) and measuring the intensity of the reflected X-rays as a function of angle.
RXR
RXRR
relative X-ray reflectivity
CHMO:0000221
relative X-ray reflectometry
A method for determining structure by directing a beam of X-rays at an extremely flat surface (at a grazing angle) and measuring the intensity of the reflected X-rays as a function of angle.
https://doi.org/10.1134/S1063785007030121
A method for determining structure by directing a beam of X-rays at an extremely flat surface (at angle theta to the surface) and measuring the intensity of the X-rays which undergo specular reflection (and are emitted at angle theta from the surface).
specular X-ray reflectivity
specular XRR
CHMO:0000222
specular X-ray reflectometry
A method for determining structure by directing a beam of X-rays at an extremely flat surface (at angle theta to the surface) and measuring the intensity of the X-rays which undergo specular reflection (and are emitted at angle theta from the surface).
https://orcid.org/0000-0002-0640-0422
Any method for determining structure where the sample is illuminated with light and the intensity and change in polarisation of the reflected light are measured.
optical ellipsometry
CHMO:0000223
ellipsometry
Any method for determining structure where the sample is illuminated with light and the intensity and change in polarisation of the reflected light are measured.
ISBN:0412581604
A method for determining structure by illuminating a sample with a monochromatic light source and measuring the intensity and change in polarisation of the reflected light.
CHMO:0000224
single-wavelength ellipsometry
A method for determining structure by illuminating a sample with a monochromatic light source and measuring the intensity and change in polarisation of the reflected light.
https://orcid.org/0000-0002-0640-0422
A method for determining structure by illuminating a sample with a continuous-wavelength light source and measuring the intensity and change in polarisation of the reflected light as a function of wavelength.
SE
spectral ellipsometry
CHMO:0000225
spectroscopic ellipsometry
A method for determining structure by illuminating a sample with a continuous-wavelength light source and measuring the intensity and change in polarisation of the reflected light as a function of wavelength.
ISBN:978-3-540-74597-6
A method for determining structure by illuminating a sample with a continuous infrared wavelength light source and measuring the intensity and change in polarisation of the reflected light as a function of wavelength.
IRSE
infra-red spectroscopic ellipsometry
infrared ellipsometric spectroscopy
CHMO:0000226
infrared spectroscopic ellipsometry
A method for determining structure by illuminating a sample with a continuous infrared wavelength light source and measuring the intensity and change in polarisation of the reflected light as a function of wavelength.
FIX:0000662
https://orcid.org/0000-0002-0640-0422
A method for determining structure by illuminating an anisotropic sample with a continous infrared wavelength light source in a magnetic field and measuring the intensity and change in polarisation of the reflected light as a function of wavelength.
MOGE
CHMO:0000227
magneto-optic generalised ellipsometry
A method for determining structure by illuminating an anisotropic sample with a continous infrared wavelength light source in a magnetic field and measuring the intensity and change in polarisation of the reflected light as a function of wavelength.
https://orcid.org/0000-0002-0640-0422
The study of the interaction of a sample with radiation or particles for measurement or detection.
spectrometry
CHMO:0000228
spectroscopy
The study of the interaction of a sample with radiation or particles for measurement or detection.
https://doi.org/10.1351/goldbook.S05848
Spectrometry where the noise generated by the movement of bubbles or particles is detected.
acoustic emission spectroscopy
CHMO:0000229
acoustic emission spectrometry
Spectrometry where the noise generated by the movement of bubbles or particles is detected.
ISBN:3527605029
Spectrometry where the alpha-particles (or 4He nuclei) spontaneously emitted from radioisotopes are detected.
alpha spectroscopy
alpha-particle spectrometry
CHMO:0000230
alpha-particle spectroscopy
Spectrometry where the alpha-particles (or 4He nuclei) spontaneously emitted from radioisotopes are detected.
https://orcid.org/0000-0002-0640-0422
true
Any spectroscopic method which probes the electronic degrees of freedom of an atom or molecule.
FIX:0000032
CHMO:0000232
electronic spectroscopy
Any spectroscopic method which probes the electronic degrees of freedom of an atom or molecule.
https://orcid.org/0000-0001-5985-7429
Any spectroscopic technique which is based upon the ability of atoms to absorb or emit electromagnetic radiation. In atomic spectroscopy the sample is vaporised and then atomised.
FIX:0000054
atomic spectrometry
CHMO:0000233
atomic spectroscopy
Any spectroscopic technique which is based upon the ability of atoms to absorb or emit electromagnetic radiation. In atomic spectroscopy the sample is vaporised and then atomised.
https://orcid.org/0000-0002-0640-0422
A type of atomic spectroscopy where the sample is illuminated with ultraviolet or visible light which is absorbed by the non-excited atoms at characteristic wavelengths.
FIX:0000926
AAS
atomic absorption spectrometry
atomic-absorption spectrometry
CHMO:0000234
atomic absorption spectroscopy
A type of atomic spectroscopy where the sample is illuminated with ultraviolet or visible light which is absorbed by the non-excited atoms at characteristic wavelengths.
ISBN:0-19-280031-0
A type of atomic absorption spectrometry where a glow discharge (a potential difference applied across two electrodes immersed in the sample gas) is used to atomise the sample before it absorbs ultra-violet or visible light atoms at characteristic wavelengths.
GD-AAS
GDAAS
atomic absorption glow-discharge spectrometry
glow discharge atomic absorption spectrometry
glow discharge atomic absorption spectroscopy
CHMO:0000235
atomic absorption glow-discharge spectroscopy
A type of atomic absorption spectrometry where a glow discharge (a potential difference applied across two electrodes immersed in the sample gas) is used to atomise the sample before it absorbs ultra-violet or visible light atoms at characteristic wavelengths.
https://doi.org/10.1366/0003702953964822
A type of atomic absorption spectrometry where no vaporisation step is required because the sample is a volatile heavy metal such as mercury, which is a vapour at room temperature.
CV-AAS
CVAAS
cold vapor AAS
cold vapor atomic absorption spectrometry
cold vapor atomic absorption spectroscopy
cold vapour AAS
CHMO:0000236
cold vapour atomic absorption spectrometry
A type of atomic absorption spectrometry where no vaporisation step is required because the sample is a volatile heavy metal such as mercury, which is a vapour at room temperature.
https://orcid.org/0000-0002-0640-0422
A type of atomic absorption spectrometry where the sample is atomised using a probe which is rapidly heated by passing a current through it.
ET-AAS
ETAAS
electrothermal atomic absorption spectroscopy
CHMO:0000237
electrothermal atomic absorption spectrometry
A type of atomic absorption spectrometry where the sample is atomised using a probe which is rapidly heated by passing a current through it.
ISSN:1430-4171
A method where a liquid sample is first separated by capillary electrophoresis, then vaporised and atomised using a probe which is rapidly heated by passing a current through it. The sample is then analysed by illuminating it with ultraviolet or visible light which is absorbed by the non-excited atoms at characteristic wavelengths.
CE-ETAAS
capillary electrophoresis electrothermal atomic absorption spectroscopy
CHMO:0000238
capillary electrophoresis-electrothermal atomic absorption spectrometry
A method where a liquid sample is first separated by capillary electrophoresis, then vaporised and atomised using a probe which is rapidly heated by passing a current through it. The sample is then analysed by illuminating it with ultraviolet or visible light which is absorbed by the non-excited atoms at characteristic wavelengths.
https://orcid.org/0000-0002-0640-0422
A type of atomic absorption spectrometry where the sample is atomised by placing it in a small graphite-coated tube which is rapidly heated by passing a current through it.
GF-AAS
GFAAS
graphite furnace atomic absorption spectroscopy
graphite-furnace atomic-absorption spectroscopy
CHMO:0000239
graphite furnace atomic absorption spectrometry
A type of atomic absorption spectrometry where the sample is atomised by placing it in a small graphite-coated tube which is rapidly heated by passing a current through it.
FIX:0000951
https://orcid.org/0000-0002-0640-0422
A type of atomic absorption spectrometry where a solid sample is ground into a fine powder and suspensed in a diluent such as 0.1% HNO3 to form a 'slurry'. The sample is then atomised by placing it in a small graphite-coated tube which is rapidly heated by passing a current through it.
slurry sampling graphite furnace atomic absorption spectroscopy
CHMO:0000240
slurry sampling graphite furnace atomic absorption spectrometry
A type of atomic absorption spectrometry where a solid sample is ground into a fine powder and suspensed in a diluent such as 0.1% HNO3 to form a 'slurry'. The sample is then atomised by placing it in a small graphite-coated tube which is rapidly heated by passing a current through it.
ISBN:1566701554
A type of atomic absorption spectrometry where a solid sample is atomised by placing it in a small graphite-coated tube which is rapidly heated by passing a current through it.
SS-GF-AAS
SS-GFAAS
direct solid samples graphite furnace atomic absorption spectrometry
direct solid samples graphite furnace atomic absorption spectroscopy
direct solid sampling graphite furnace atomic absorption spectrometry
direct solid sampling graphite furnace atomic absorption spectroscopy
solid samples graphite furnace atomic absorption spectrometry
solid samples graphite furnace atomic absorption spectroscopy
solid sampling graphite furnace atomic absorption spectrometry
CHMO:0000241
solid sampling graphite furnace atomic absorption spectrometry
A type of atomic absorption spectrometry where a solid sample is atomised by placing it in a small graphite-coated tube which is rapidly heated by passing a current through it.
https://orcid.org/0000-0002-0640-0422
A type of atomic absorption spectrometry where a solid sample is atomised by placing it in a small quartz tube which is rapidly heated by passing a current through it.
QT-AAS
QTAAS
quartz tube atomic absorption spectrometry
CHMO:0000242
quartz tube atomic absorption spectroscopy
A type of atomic absorption spectrometry where a solid sample is atomised by placing it in a small quartz tube which is rapidly heated by passing a current through it.
https://doi.org/JA9900500225
A type of atomic absorption spectrometry where the sample is aspirated, aerosolised, and mixed with combustible gases, such as acetylene and air or acetylene and nitrous oxide. The mixture is then ignited and atomised in a flame whose temperature ranges from 2100–2800 \degC. During combustion, atoms of the element of interest in the sample absorb light at characteristic wavelengths.
F-AAS
FAAS
flame atomic absorption spectroscopy
CHMO:0000243
flame atomic absorption spectrometry
A type of atomic absorption spectrometry where the sample is aspirated, aerosolised, and mixed with combustible gases, such as acetylene and air or acetylene and nitrous oxide. The mixture is then ignited and atomised in a flame whose temperature ranges from 2100–2800 \degC. During combustion, atoms of the element of interest in the sample absorb light at characteristic wavelengths.
FIX:0000929
https://orcid.org/0000-0002-0640-0422
A type of atomic absorption spectrometry where sample is forced through a heated metal capillary tip before atomisation in a flame.
(TS-FF)-AAS
TS-FF-AAS
thermospray flame furnace atomic absorption spectroscopy
CHMO:0000244
thermospray flame furnace atomic absorption spectrometry
A type of atomic absorption spectrometry where sample is forced through a heated metal capillary tip before atomisation in a flame.
https://doi.org/10.1016/S0584-8547(00)00183-X
A type of atomic absorption spectrometry where the sample is carried to the spectrometer by flow injection and forced through a heated metal capillary tip before atomisation in a flame furnace.
FI-TS-FF-AAS
flow injection thermospray flame furnace absorption spectrometry
CHMO:0000245
flow injection thermospray flame furnace absorption spectrometry
A type of atomic absorption spectrometry where the sample is carried to the spectrometer by flow injection and forced through a heated metal capillary tip before atomisation in a flame furnace.
https://orcid.org/0000-0002-0640-0422
A type of atomic absorption spectrometry where flow injection is used to transfer a sample to the spectrometer.
FI-AAS
FIAAS
flow injection atomic absorption spectroscopy
CHMO:0000246
flow injection atomic absorption spectrometry
A type of atomic absorption spectrometry where flow injection is used to transfer a sample to the spectrometer.
https://orcid.org/0000-0002-0640-0422
A type of atomic absorption spectrometry where flow injection is used to carry a sample to an electrothermal atomiser where it is atomised using a probe which is rapidly heated by passing a current through it.
FI-ETAAS
FIETAAS
flow injection electrothermal atomic absorption spectrometry
flow injection electrothermal atomisation atomic absorption spectrometry
flow injection electrothermal atomization atomic absorption spectrometry
flow injection electrothermal atomization atomic absorption spectroscopy
CHMO:0000247
flow injection electrothermal atomic absorption spectrometry
A type of atomic absorption spectrometry where flow injection is used to carry a sample to an electrothermal atomiser where it is atomised using a probe which is rapidly heated by passing a current through it.
https://orcid.org/0000-0002-0640-0422
A type of atomic absorption spectrometry where flow injection is used to carry a gas phase sample to flame where it is atomised.
FI-FAAS
FIFAAS
flow injection flame atomic absorption spectrometry
CHMO:0000248
flow injection flame atomic absorption spectrometry
A type of atomic absorption spectrometry where flow injection is used to carry a gas phase sample to flame where it is atomised.
https://orcid.org/0000-0002-0640-0422
A type of atomic absorption spectrometry where metal samples such as As, Sb and Se are vaporised by converting them into volatile hydrides.
HG-AAS
HGAAS
hydride generation atomic absorption spectrometry
hydride-generation atomic absorption spectrometry
CHMO:0000249
hydride generation atomic absorption spectroscopy
A type of atomic absorption spectrometry where metal samples such as As, Sb and Se are vaporised by converting them into volatile hydrides.
https://orcid.org/0000-0002-0640-0422
A type of atomic absorption spectrometry using a line source of radiation.
LS-AAS
LSAAS
line source atomic absorption spectrometry
CHMO:0000250
line-source atomic absorption spectroscopy
A type of atomic absorption spectrometry using a line source of radiation.
https://orcid.org/0000-0002-0640-0422
A type of atomic spectroscopy where the atoms in the sample are excited and the emission of electromagnetic radiation at characteristic wavelengths is detected.
FIX:0000927
AES
OES
atomic emission spectrometry
atomic-emission spectrometry
optical emission spectrometry
optical emission spectroscopy
CHMO:0000251
atomic emission spectroscopy
A type of atomic spectroscopy where the atoms in the sample are excited and the emission of electromagnetic radiation at characteristic wavelengths is detected.
ISBN:0-19-280031-0
A type of atomic emission spectrometry where the sample is atomised using a probe which is rapidly heated by passing a current through it.
ETAES
electrothermal atomic emission spectrometry
CHMO:0000252
electrothermal atomic emission spectroscopy
A type of atomic emission spectrometry where the sample is atomised using a probe which is rapidly heated by passing a current through it.
https://orcid.org/0000-0002-0640-0422
A type of atomic emission spectrometry where the sample is atomised by placing it in a small graphite-coated tube which is rapidly heated by passing a current through it.
GF-AES
GF-OES
GFAES
GFOES
graphite furnace atomic emission spectrometry
graphite furnace optical emission spectrometry
graphite furnace optical emission spectroscopy
CHMO:0000253
graphite furnace atomic emission spectrometry
A type of atomic emission spectrometry where the sample is atomised by placing it in a small graphite-coated tube which is rapidly heated by passing a current through it.
https://orcid.org/0000-0002-0640-0422
A type of atomic emission spectrometry where the sample is atomised by placing it in a small graphite-coated tube which is rapidly heated by passing a current through it, then excited using a glow discharge (a potential difference applied across two electrodes immersed in the sample gas).
FANES
furnace atomic non thermal excitation spectrometry
furnace atomic non-thermal excitation spectrometry
furnace atomic non-thermal excitation spectroscopy
furnace atomic nonthermal excitation spectroscopy
CHMO:0000254
furnace atomic nonthermal excitation spectrometry
A type of atomic emission spectrometry where the sample is atomised by placing it in a small graphite-coated tube which is rapidly heated by passing a current through it, then excited using a glow discharge (a potential difference applied across two electrodes immersed in the sample gas).
ISBN:0471974188
A type of atomic emission spectrometry where the sample is excited using an N2/oxide–acetylene flame.
F-AES
FAES
flame atomic emission spectroscopy
flame emission spectroscopy
CHMO:0000255
flame atomic emission spectroscopy
A type of atomic emission spectrometry where the sample is excited using an N2/oxide–acetylene flame.
FIX:0000928
FIX:0000935
https://doi.org/10.1039/ja9870200573
A type of atomic emission spectrometry where a glow discharge (a potential difference applied across two electrodes immersed in the sample gas) is used to excite the sample.
GD-AES
GD-OES
glow discharge optical emission spectrometry
glow discharge optical emission spectroscopy
CHMO:0000256
glow discharge atomic emission spectroscopy
A type of atomic emission spectrometry where a glow discharge (a potential difference applied across two electrodes immersed in the sample gas) is used to excite the sample.
https://orcid.org/0000-0002-0640-0422
A type of atomic emission spectrometry where a laser pulse is used as the excitation source.
LIP AES
LIP-AES
laser-induced atomic emission spectrometry
CHMO:0000257
laser-induced atomic emission spectroscopy
A type of atomic emission spectrometry where a laser pulse is used as the excitation source.
https://orcid.org/0000-0002-0640-0422
A type of atomic emission spectrometry where a high energy laser pulse is used to generate a plasma which acts as the excitation source.
LIBS
LIPS
laser induced plasma spectrometry
laser induced plasma spectroscopy
laser-induced breakdown atomic emission spectrometry
laser-induced breakdown atomic-emission spectrometry
laser-induced plasma atomic emission spectrometry
laser-induced plasma atomic emission spectroscopy
laser-induced plasma spectrometry
laser-induced plasma spectroscopy
CHMO:0000258
laser-induced breakdown spectroscopy
A type of atomic emission spectrometry where a high energy laser pulse is used to generate a plasma which acts as the excitation source.
https://orcid.org/0000-0002-0640-0422
A type of atomic emission spectrometry where a high energy femtosecond laser pulse is used to generate a plasma which acts as the excitation source.
fs-LIBS
CHMO:0000259
femtosecond laser-induced breakdown spectroscopy
A type of atomic emission spectrometry where a high energy femtosecond laser pulse is used to generate a plasma which acts as the excitation source.
https://orcid.org/0000-0002-0640-0422
A type of atomic emission spectrometry where a high energy laser pulse is used to generate a plasma which acts as the excitation source. A second laser pulse then illuminates the sample resulting in a reheating of the laser plasma produced by the first pulse, leading to signal enhancement.
LISPS
double-pulse LIBS
double-pulse laser-induced breakdown spectrometry
double-pulse laser-induced breakdown spectroscopy
laser-induced shock wave spectrometry
CHMO:0000260
laser-induced shock wave plasma spectroscopy
A type of atomic emission spectrometry where a high energy laser pulse is used to generate a plasma which acts as the excitation source. A second laser pulse then illuminates the sample resulting in a reheating of the laser plasma produced by the first pulse, leading to signal enhancement.
https://orcid.org/0000-0002-0640-0422
A type of atomic emission spectrometry where a finely focused (<10 m diameter) high energy laser pulse is used to generate a plasma which acts as the excitation source.
micro LIBS
CHMO:0000261
micro laser-induced breakdown atomic emission spectroscopy
A type of atomic emission spectrometry where a finely focused (<10 m diameter) high energy laser pulse is used to generate a plasma which acts as the excitation source.
https://orcid.org/0000-0002-0640-0422
A type of atomic emission spectrometry where a high energy nanosecond laser pulse is used to generate a plasma which acts as the excitation source.
nanosecond LIBS
nanosecond laser induced breakdown spectrometry
ns-LIBS
CHMO:0000262
nanosecond laser-induced breakdown spectroscopy
A type of atomic emission spectrometry where a high energy nanosecond laser pulse is used to generate a plasma which acts as the excitation source.
https://orcid.org/0000-0002-0640-0422
Any type of atomic emission spectrometry where a plasma is used as the excitation source.
plasma AES
CHMO:0000263
plasma atomic emission spectroscopy
Any type of atomic emission spectrometry where a plasma is used as the excitation source.
ISSN:1430-4171
A type of atomic emission spectrometry where a plasma generated by a potential difference between two electrodes, one of which is grounded and one of which is live.
CCP AES
CCP-AES
capacitively coupled plasma atomic emission spectrometry
CHMO:0000264
capacitively coupled plasma atomic emission spectroscopy
A type of atomic emission spectrometry where a plasma generated by a potential difference between two electrodes, one of which is grounded and one of which is live.
https://orcid.org/0000-0002-0640-0422
A type of atomic emission spectrometry where a plasma generated by passing an electrical discharge between two electrodes is used as the excitation source.
DCP-AES
DCPAES
d.c. AES
d.c. plasma atomic emission spectrometry
d.c. plasma atomic emission spectroscopy
direct current plasma atomic emission spectrometry
CHMO:0000265
direct current plasma atomic emission spectroscopy
A type of atomic emission spectrometry where a plasma generated by passing an electrical discharge between two electrodes is used as the excitation source.
https://orcid.org/0000-0002-0640-0422
A type of atomic emission spectrometry where a furnace is used to atomise the sample and a plasma is used as the excitation source.
FAPES
furnace atomisation plasma emission spectrometry
furnace atomization plasma emission spectrometry
CHMO:0000266
furnace atomisation plasma emission spectroscopy
A type of atomic emission spectrometry where a furnace is used to atomise the sample and a plasma is used as the excitation source.
ISBN:0471974188
A type of atomic emission spectrometry where a plasma generated by electromagnetic induction is used as the excitation source.
ICP AES
ICP OES
ICP-AES
ICP-OES
inductively coupled plasma atomic emission spectrometry
inductively coupled plasma atomic emission spectroscopy
inductively coupled plasma atomic-emission spectrometry
inductively coupled plasma optical emission spectrometry
inductively coupled plasma optical emission spectroscopy
inductively coupled plasma-atomic emission spectrometry
inductively coupled plasma-atomic emission spectroscopy
inductively coupled plasma-optical emission spectrometry
inductively coupled plasma-optical emission spectroscopy
CHMO:0000267
inductively-coupled plasma atomic emission spectroscopy
A type of atomic emission spectrometry where a plasma generated by electromagnetic induction is used as the excitation source.
ISSN:1430-4171
Atomic emission spectrometry of metal samples such as As, Sb and Se that are vaporised by converting them into volatile hydrides and excited using a plasma generated by electromagnetic induction.
HG-ICP-AES
HG-ICP-OES
hydride generation inductively coupled plasma atomic emission spectrometry
hydride generation inductively coupled plasma optical emission spectrometry
hydride generation inductively coupled plasma optical emission spectroscopy
CHMO:0000268
hydride generation inductively coupled plasma atomic emission spectroscopy
Atomic emission spectrometry of metal samples such as As, Sb and Se that are vaporised by converting them into volatile hydrides and excited using a plasma generated by electromagnetic induction.
https://orcid.org/0000-0002-0640-0422
Inductively coupled atomic emission spectrometry where the sample is vaporised by laser ablation.
LA ICP AES
LA ICP-AES
laser ablation ICP AES
laser ablation inductively coupled plasma atomic emission spectrometry
CHMO:0000269
laser ablation inductively-coupled plasma atomic emission spectroscopy
Inductively coupled atomic emission spectrometry where the sample is vaporised by laser ablation.
https://orcid.org/0000-0002-0640-0422
Inductively coupled atomic emission spectrometry where the sample is vaporised by laser ablation with a finely focused (<10 m diameter) laser.
LM-ICP-AES
laser microprobe ICP-AES
CHMO:0000270
laser microprobe inductively coupled plasma atomic emission spectroscopy
Inductively coupled atomic emission spectrometry where the sample is vaporised by laser ablation with a finely focused (<10 m diameter) laser.
https://orcid.org/0000-0002-0640-0422
Inductively coupled plasma atomic emission spectroscopy where the sample mixture is first separated by liquid chromatography.
LC-ICP-AES
LC-ICP-OES
liquid chromatography inductively coupled plasma atomic emission spectrometry
liquid chromatography inductively coupled plasma atomic emission spectroscopy
liquid chromatography inductively coupled plasma optical emission spectrometry
liquid chromatography inductively coupled plasma optical emission spectroscopy
CHMO:0000271
liquid chromatography-inductively coupled plasma atomic emission spectroscopy
Inductively coupled plasma atomic emission spectroscopy where the sample mixture is first separated by liquid chromatography.
https://orcid.org/0000-0002-0640-0422
Inductively-coupled atomic emission spectrometry where the sample mixture is first passed through a nebuliser to form a mist of finely dispersed droplets using compressed air.
nebulisation inductively coupled plasma atomic emission spectrometry
nebulization inductively coupled plasma atomic emission spectrometry
nebulization inductively coupled plasma atomic emission spectroscopy
CHMO:0000272
nebulisation inductively-coupled plasma atomic emission spectroscopy
Inductively-coupled atomic emission spectrometry where the sample mixture is first passed through a nebuliser to form a mist of finely dispersed droplets using compressed air.
https://orcid.org/0000-0002-0640-0422
A type of atomic emission spectrometry where the sample mixture is first passed through a nebuliser to form a mist of finely dispersed droplets (using high frequency vibrations) and then excited using a plasma generated by electromagnetic inductance.
USN-ICP-AES
USN-ICP-OES
ultrasonic nebulisation inductively coupled plasma atomic emission spectrometry
ultrasonic nebulisation inductively coupled plasma optical emission spectrometry
ultrasonic nebulisation inductively coupled plasma optical emission spectroscopy
ultrasonic nebulization inductively coupled plasma atomic emission spectrometry
ultrasonic nebulization inductively coupled plasma atomic emission spectroscopy
ultrasonic nebulization inductively coupled plasma optical emission spectrometry
ultrasonic nebulization inductively coupled plasma optical emission spectroscopy
CHMO:0000273
ultrasonic nebulisation inductively coupled plasma atomic emission spectroscopy
A type of atomic emission spectrometry where the sample mixture is first passed through a nebuliser to form a mist of finely dispersed droplets (using high frequency vibrations) and then excited using a plasma generated by electromagnetic inductance.
https://orcid.org/0000-0002-0640-0422
A type of atomic emission spectrometry where the sample mixture is first separated by solid phase extraction and then excited using a plasma generated by electromagnetic inductance.
SPE-ICP-AES
CHMO:0000274
solid phase extraction inductively coupled plasma atomic emission spectroscopy
A type of atomic emission spectrometry where the sample mixture is first separated by solid phase extraction and then excited using a plasma generated by electromagnetic inductance.
https://orcid.org/0000-0002-0640-0422
A type of atomic emission spectrometry where the sample mixture is first separated by solid phase extraction, carried to the spectrometer by flow injection and then excited using a plasma generated by electromagnetic inductance.
FI-SPE-ICP-AES
CHMO:0000275
flow injection solid phase extraction inductively coupled plasma atomic emission spectroscopy
A type of atomic emission spectrometry where the sample mixture is first separated by solid phase extraction, carried to the spectrometer by flow injection and then excited using a plasma generated by electromagnetic inductance.
https://orcid.org/0000-0002-0640-0422
A type of atomic emission spectrometry where atoms are excited by energy transfer from metastable N2 species in a nitrogen plasma.
MTES
metastable transfer emission spectroscopy
CHMO:0000276
metastable transfer emission spectrometry
A type of atomic emission spectrometry where atoms are excited by energy transfer from metastable N2 species in a nitrogen plasma.
https://doi.org/10.1021/ac00248a042
Atomic emission spectrometry where a plasma generated by microwave bombardment is used as the excitation source.
FIX:0000931
MIP AES
MIP-AES
microwave-induced plasma atomic emission spectroscopy
CHMO:0000277
microwave induced plasma atomic emission spectrometry
Atomic emission spectrometry where a plasma generated by microwave bombardment is used as the excitation source.
ISSN:1430-4171
Atomic emission spectrometry where the sample is excited by an arc or spark between two electrodes.
spark AES
spark OES
spark atomic emission spectroscopy
spark optical emission spectrometry
spark optical emission spectroscopy
spark-AES
spark-OES
spark-atomic emission spectrometry
spark-excitation atomic emission spectrometry
spark-excitation atomic emission spectroscopy
spark-optical emission spectrometry
spark-optical emission spectroscopy
CHMO:0000278
spark atomic emission spectrometry
Atomic emission spectrometry where the sample is excited by an arc or spark between two electrodes.
https://orcid.org/0000-0002-0640-0422
Atomic spectroscopy where an atom absorbs then spontaneously emits a photon.
FIX:0000290
AFS
atomic fluorescence spectrometry
atomic-fluorescence spectrometry
CHMO:0000279
atomic fluorescence spectroscopy
Atomic spectroscopy where an atom absorbs then spontaneously emits a photon.
https://orcid.org/0000-0002-0640-0422
Atomic fluorescence spectroscopy where no vaporisation step is required because the sample is a volatile heavy metal such as mercury, which is a vapour at room temperature.
CV-AFS
CVAFS
cold vapor AFS
cold vapor atomic fluorescence spectrometry
cold vapor atomic fluorescence spectroscopy
cold vapour AFS
cold vapour atomic fluorescence spectrometry
CHMO:0000280
cold vapour atomic fluorescence spectroscopy
Atomic fluorescence spectroscopy where no vaporisation step is required because the sample is a volatile heavy metal such as mercury, which is a vapour at room temperature.
https://orcid.org/0000-0002-0640-0422
Atomic fluorescence spectroscopy where the sample is atomised using a probe which is rapidly heated by passing a current through it.
ETAFS
electrothermal atomic fluorescence spectrometry
CHMO:0000281
electrothermal atomic fluorescence spectroscopy
Atomic fluorescence spectroscopy where the sample is atomised using a probe which is rapidly heated by passing a current through it.
https://orcid.org/0000-0002-0640-0422
A type of atomic fluorescence spectroscopy where the sample is atomised using a flame.
FAFS
FFS
flame atomic fluorescence spectrometry
flame fluorescence spectrometry
flame fluorescence spectroscopy
CHMO:0000282
flame atomic fluorescence spectroscopy
A type of atomic fluorescence spectroscopy where the sample is atomised using a flame.
FIX:0000930
https://orcid.org/0000-0002-0640-0422
A type of atomic fluorescence spectroscopy of metal samples such as As, Sb and Se which are vaporised by converting them into volatile hydrides.
HG-AFS
HGAFS
hydride generation atomic fluorescence spectrometry
CHMO:0000283
hydride generation atomic fluorescence spectroscopy
A type of atomic fluorescence spectroscopy of metal samples such as As, Sb and Se which are vaporised by converting them into volatile hydrides.
https://orcid.org/0000-0002-0640-0422
A type of atomic fluorescence spectroscopy where a laser is used to excite the atoms in the sample.
LEAF
LEAFS
laser-enhanced atomic fluorescence spectrometry
laser-excited atomic fluorescence spectrometry
laser-excited atomic fluorescence spectroscopy
CHMO:0000284
laser-enhanced atomic fluorescence spectroscopy
A type of atomic fluorescence spectroscopy where a laser is used to excite the atoms in the sample.
https://orcid.org/0000-0002-0640-0422
A type of atomic fluorescence spectroscopy where a plasma is used to excite the atoms in the sample.
plasma AFS
plasma atomic fluorescence spectrometry
CHMO:0000285
plasma atomic fluorescence spectroscopy
A type of atomic fluorescence spectroscopy where a plasma is used to excite the atoms in the sample.
https://orcid.org/0000-0002-0640-0422
A type of atomic fluorescence spectroscopy where a plasma generated by electromagnetic induction is used to excite the atoms in the sample.
ICP AFS
inductively coupled plasma atomic fluorescence spectroscopy
CHMO:0000286
inductively coupled plasma atomic fluorescence spectrometry
A type of atomic fluorescence spectroscopy where a plasma generated by electromagnetic induction is used to excite the atoms in the sample.
https://orcid.org/0000-0002-0640-0422
Spectroscopy where the intensity of the fluorescence emitted by molecules excited by ultraviolet light is detected as a function of wavelength or time.
fluorescence emission spectroscopy
fluorescence spectrometry
fluorescence spectrophotometry
fluorimetry
fluorometry
spectrofluorimetry
spectrofluorometry
CHMO:0000287
fluorescence spectroscopy
Spectroscopy where the intensity of the fluorescence emitted by molecules excited by ultraviolet light is detected as a function of wavelength or time.
FIX:0000028
https://orcid.org/0000-0002-0640-0422
Spectroscopy where the spontaneous fluorescence intensity fluctuations of a sample are measured and correlated within a very small detection volume. Ultraviolet light is used to stimulate fluorescence.
FCS
fluroescence correlation spectrometry
CHMO:0000288
fluorescence correlation spectroscopy
Spectroscopy where the spontaneous fluorescence intensity fluctuations of a sample are measured and correlated within a very small detection volume. Ultraviolet light is used to stimulate fluorescence.
FIX:0000352
https://doi.org/10.1039/b718132a
Spectroscopy where spontaneous fluorescence intensity fluctuations of a sample are measured at two distinct wavelengths and correlated within a very small detection volume. Ultra-violet light is used to stimulate fluorescence.
FCCS
fluorescence cross-correlation spectrometry
CHMO:0000289
fluorescence cross-correlation spectroscopy
Spectroscopy where spontaneous fluorescence intensity fluctuations of a sample are measured at two distinct wavelengths and correlated within a very small detection volume. Ultra-violet light is used to stimulate fluorescence.
https://orcid.org/0000-0002-0640-0422
A method for measuring the binding interaction between two labelled molecules. The sample is excited with vertically polarised light and the polarization of the fluorescence is measured.
FIX:0000128
FA
fluorescence anisotropy measurement
fluorescence polarisation spectroscopy
fluorescence polarization spectroscopy
CHMO:0000290
fluorescence anisotropy
A method for measuring the binding interaction between two labelled molecules. The sample is excited with vertically polarised light and the polarization of the fluorescence is measured.
https://orcid.org/0000-0002-0640-0422
Spectroscopy where the sample absorbs radiation in the range ultraviolet to near-infrared (0.1–2.5 μm) resulting in electronic transitions within the sample.
FIX:0000011
FIX:0000943
molecular absorption spectrophotometry
molecular electronic absorption spectroscopy
MAS
CHMO:0000291
spectrophotometry
Spectroscopy where the sample absorbs radiation in the range ultraviolet to near-infrared (0.1–2.5 μm) resulting in electronic transitions within the sample.
ISBN:1566701783
MAS
Spectroscopy where the sample absorbs radiation in the range ultraviolet to visible (190-800 nm) resulting in electronic transitions within the sample.
FIX:0000016
UV spectrometry
UV-VIS
UV-VIS absorption spectrophotometry
UV-VIS absorption spectroscopy
UV-VIS spectrophotometry
UV-VIS spectroscopy
UV-Vis molecular absorption spectrometry
UV-Vis molecular absorption spectroscopy
UV-Vis spectroscopy
UV-vis
UV-vis absorption spectrometry
UV-vis absorption spectrophotometry
UV-vis absorption spectroscopy
UV-vis spectrometry
UV-vis spectrophotometry
UV-vis spectroscopy
UV-visible
UV-visible spectroscopy
UV/VIS
UV/VIS absorption spectrophotometry
UV/VIS spectrometry
UV/VIS spectrophotometry
UV/VIS spectroscopy
UV/Vis absorption spectrophotometry
UV/Vis spectrometry
UV/Vis spectrophotometry
UV/Vis spectroscopy
UV/vis
absorption spectrophotometry
electronic absorption spectroscopy
ultra-violet-visible absorption spectrophotometry
ultra-violet-visible spectrometry
ultra-violet-visible spectroscopy
ultraviolet-visible
ultraviolet-visible spectrometry
ultraviolet-visible spectrophotometry
ultraviolet-visible spectroscopy
CHMO:0000292
ultraviolet-visible spectrophotometry
Spectroscopy where the sample absorbs radiation in the range ultraviolet to visible (190-800 nm) resulting in electronic transitions within the sample.
https://orcid.org/0000-0002-0640-0422
Ultraviolet-visible spectroscopy where the difference between incident and transmitted radiation is measured for a gaseous sample.
DOAS
differential optical absorbance spectrometry
differential optical absorbance spectroscopy
differential optical absorption spectrometry
differential optical absorption spectroscopy
CHMO:0000293
differential optical absorption spectrophotometry
Ultraviolet-visible spectroscopy where the difference between incident and transmitted radiation is measured for a gaseous sample.
https://orcid.org/0000-0002-0640-0422
Ultraviolet–visible spectroscopy where the reflection or scattering of radiation from the sample surface is detected.
reflectance UV-VIS spectrometry
reflectance UV-VIS spectroscopy
reflectance UV/VIS spectrometry
reflectance UV/VIS spectroscopy
reflectance ultra-violet-visible spectrometry
reflectance ultra-violet-visible spectroscopy
reflectance ultra-violet–visible spectrophotometry
reflectance ultraviolet-visible spectroscopy
reflection UV-VIS spectrometry
reflection UV-VIS spectroscopy
reflection UV/VIS spectrometry
reflection UV/VIS spectroscopy
reflection ultra-violet-visible spectrometry
reflection ultra-violet-visible spectroscopy
reflection ultraviolet-visible spectrometry
reflection ultraviolet-visible spectroscopy
ultra-violet-visible reflectance spectrometry
CHMO:0000294
reflectance ultraviolet-visible spectrophotometry
Ultraviolet–visible spectroscopy where the reflection or scattering of radiation from the sample surface is detected.
https://orcid.org/0000-0002-0640-0422
A method where the absorption of radiation in the ultraviolet to near-infrared (0.1-2.5 μm) is used to calculate stability constants by equimolar dilution.
CHMO:0000295
equimolar spectrophotometry
A method where the absorption of radiation in the ultraviolet to near-infrared (0.1-2.5 μm) is used to calculate stability constants by equimolar dilution.
https://doi.org/10.1021/ac60353a044
Spectroscopy where the sample absorbs radiation in the vacuum ultraviolet region (0.1-200 nm) resulting in electronic transitions within the sample.
VUV spectrometry
VUV spectrophotometry
VUV spectroscopy
vacuum ultra-violet absorption spectrometry
vacuum ultra-violet absorption spectroscopy
vacuum ultra-violet spectrophotometry
vacuum ultraviolet absorption spectrometry
vacuum ultraviolet absorption spectroscopy
vacuum ultraviolet spectrophotometry
CHMO:0000296
vacuum ultraviolet spectrophotometry
Spectroscopy where the sample absorbs radiation in the vacuum ultraviolet region (0.1-200 nm) resulting in electronic transitions within the sample.
https://orcid.org/0000-0002-0640-0422
Spectroscopy where the absorption or emission of X-rays is detected.
X-ray spectrometry
CHMO:0000297
X-ray spectroscopy
Spectroscopy where the absorption or emission of X-rays is detected.
FIX:0000019
https://doi.org/10.1351/goldbook.X06718
Spectroscopy where the sample is bombarded with X-rays and the X-ray absorption coefficient of the sample is measured. When the incident X-ray energy matches the binding energy of an electron in an atom there is a decrease in the intensity of transmitted X-rays resulting in an absorption edge.
X-ray absorption spectrometry
XAS
CHMO:0000298
X-ray absorption spectroscopy
Spectroscopy where the sample is bombarded with X-rays and the X-ray absorption coefficient of the sample is measured. When the incident X-ray energy matches the binding energy of an electron in an atom there is a decrease in the intensity of transmitted X-rays resulting in an absorption edge.
FIX:0000107
https://orcid.org/0000-0002-0640-0422
X-ray absorption spectroscopy where changes in the X-ray absorption coefficient around the absorption edge (the part of the spectrum where the incident X-ray energy matches the binding energy of an electron) are measured as a function of incident X-ray energy.
X-ray absorption fine structure (EXAFS) measurements
X-ray absorption fine structure spectrometry
XAFS
CHMO:0000299
X-ray absorption fine structure spectroscopy
X-ray absorption spectroscopy where changes in the X-ray absorption coefficient around the absorption edge (the part of the spectrum where the incident X-ray energy matches the binding energy of an electron) are measured as a function of incident X-ray energy.
https://orcid.org/0000-0002-0640-0422
X-ray absorption spectroscopy where changes in the X-ray absorption coefficient measured 500–1000 eV below the absorption edge (the part of the spectrum where the incident X-ray energy matches the binding energy of an electron) are determined as a function of incident X-ray energy.
EXAFS
EXAFS spectrometry
EXAFS spectroscopy
EXAFSS
extended X-ray absorption fine structure spectrometry
CHMO:0000300
extended X-ray absorption fine structure spectroscopy
X-ray absorption spectroscopy where changes in the X-ray absorption coefficient measured 500–1000 eV below the absorption edge (the part of the spectrum where the incident X-ray energy matches the binding energy of an electron) are determined as a function of incident X-ray energy.
FIX:0000106
https://orcid.org/0000-0002-0640-0422
X-ray absorption spectroscopy where changes in the X-ray absorption coefficient measured 500–1000 eV below the absorption edge (the part of the spectrum where the incident X-ray energy matches the binding energy of an electron) are determined as a function of incident X-ray energy. A monochromator is scanned continuously and rapidly around the absorption edge resulting in measurement times of seconds (normal EXAFS measurements take minutes).
QEXAFS spectrometry
QEXAFS spectroscopy
QEXAFSS
quick extended X-ray absorption fine structure spectrometry
quick-scanning EXAFS
quick-scanning EXAFSS
quick-scanning extended X-ray absorption fine structure spectrometry
quick-scanning extended X-ray absorption fine structure spectroscopy
CHMO:0000301
quick extended X-ray absorption fine structure spectroscopy
X-ray absorption spectroscopy where changes in the X-ray absorption coefficient measured 500–1000 eV below the absorption edge (the part of the spectrum where the incident X-ray energy matches the binding energy of an electron) are determined as a function of incident X-ray energy. A monochromator is scanned continuously and rapidly around the absorption edge resulting in measurement times of seconds (normal EXAFS measurements take minutes).
https://doi.org/10.1107/S0909049508023327
X-ray absorption spectroscopy where changes in the X-ray absorption coefficient measured 500–1000 eV below the absorption edge (the part of the spectrum where the incident X-ray energy matches the binding energy of an electron) are determined as a function of incident X-ray energy. Measurements are taken under total reflection conditions.
REFLEXAFS
REFLEXAFS spectrometry
REFLEXAFS spectroscopy
reflEXAFS
reflEXAFSS
reflection extended X-ray absorption fine structure spectrometry
CHMO:0000302
reflection extended X-ray absorption fine structure spectroscopy
X-ray absorption spectroscopy where changes in the X-ray absorption coefficient measured 500–1000 eV below the absorption edge (the part of the spectrum where the incident X-ray energy matches the binding energy of an electron) are determined as a function of incident X-ray energy. Measurements are taken under total reflection conditions.
https://doi.org/10.1021/la025564q
X-ray absorption spectroscopy where changes in the X-ray absorption coefficient and the Auger emission of the sample are measured 500–1000 eV below the absorption edge (the part of the spectrum where the incident X-ray energy matches the binding energy of an electron) as a function of incident X-ray energy.
SEXAFS
SEXAFS spectrometry
SEXAFS spectroscopy
SEXAFSS
CHMO:0000303
surface extended X-ray absorption fine structure spectroscopy
X-ray absorption spectroscopy where changes in the X-ray absorption coefficient and the Auger emission of the sample are measured 500–1000 eV below the absorption edge (the part of the spectrum where the incident X-ray energy matches the binding energy of an electron) as a function of incident X-ray energy.
FIX:0000686
https://orcid.org/0000-0002-0640-0422
X-ray absorption spectroscopy where changes in the X-ray absorption coefficient around the absorption edge (the part of the spectrum where the incident X-ray energy matches the binding energy of an electron) are measured as a function of incident X-ray energy. Measurements are taken under total reflection conditions.
TR-XAFS
TR-XAFSS
TRXAFS
TRXAFSS
total-reflection X-ray absorption fine structure spectrometry
CHMO:0000304
total-reflection X-ray absorption fine structure spectroscopy
X-ray absorption spectroscopy where changes in the X-ray absorption coefficient around the absorption edge (the part of the spectrum where the incident X-ray energy matches the binding energy of an electron) are measured as a function of incident X-ray energy. Measurements are taken under total reflection conditions.
https://orcid.org/0000-0002-0640-0422
X-ray absorption spectroscopy where changes in the X-ray absorption coefficient measured within 40 eV of the absorption edge (the part of the spectrum where the incident X-ray energy matches the binding energy of an electron) are determined as a function of incident X-ray energy.
NEXAF spectroscopy
NEXAFS
NEXAFS spectrometry
NEXAFSS
X-ray absorption near edge structure (XANES) spectroscopy
X-ray absorption near edge structure spectrometry
X-ray absorption near edge structure spectroscopy
X-ray absorption near-edge structure
XANES
XANES spectrometry
XANES spectroscopy
near edge X-ray absorption spectroscopy
near-edge X-ray absorption fine structure spectrometry
CHMO:0000305
near-edge X-ray absorption fine structure spectroscopy
X-ray absorption spectroscopy where changes in the X-ray absorption coefficient measured within 40 eV of the absorption edge (the part of the spectrum where the incident X-ray energy matches the binding energy of an electron) are determined as a function of incident X-ray energy.
FIX:0000025
FIX:0000376
https://orcid.org/0000-0002-0640-0422
Spectroscopy where the sample is bombarded with a finely focused X-ray beam (<10 m diameter) and the X-ray absorption coefficient of the sample is measured.
X-ray micro-probe spectrometry
X-ray microanalysis
X-ray microprobe spectrometry
X-ray microprobe spectroscopy
XMPS
CHMO:0000306
X-ray microprobe spectroscopy
Spectroscopy where the sample is bombarded with a finely focused X-ray beam (<10 m diameter) and the X-ray absorption coefficient of the sample is measured.
https://orcid.org/0000-0002-0640-0422
X-ray spectroscopy where the sample is bombarded with X-rays or particles and the energies and intensities of the X-rays emitted due to core-to-core transitions (known as 'X-ray fluorescence') are detected.
X-ray emission spectrometry
X-ray fluorescence spectrometry
X-ray fluorescence spectroscopy
XES
XRES
XRF
XRF spectrometry
XRF spectroscopy
CHMO:0000307
X-ray emission spectroscopy
X-ray spectroscopy where the sample is bombarded with X-rays or particles and the energies and intensities of the X-rays emitted due to core-to-core transitions (known as 'X-ray fluorescence') are detected.
FIX:0000100
FIX:0000673
ISBN:90190280031-0
X-ray emission spectroscopy where the sample is irradiated with alpha-particles and the energies of the backscattered alpha-particles and X-rays emitted due to core-to-core transitions are measured.
APXS
alpha X-ray spectrometry
alpha X-ray spectroscopy
alpha-X-ray emission spectrometry
alpha-X-ray emission spectroscopy
alpha-X-ray fluorescence spectrometry
alpha-X-ray fluorescence spectroscopy
alpha-X-ray spectrometry
alpha-X-ray spectroscopy
alpha-particle X-ray emission spectrometry
alpha-particle X-ray emission spectroscopy
alpha-particle X-ray fluorescence spectrometry
alpha-particle X-ray fluorescence spectroscopy
alpha-particle X-ray spectrometry
CHMO:0000308
alpha-particle X-ray spectroscopy
X-ray emission spectroscopy where the sample is irradiated with alpha-particles and the energies of the backscattered alpha-particles and X-rays emitted due to core-to-core transitions are measured.
https://orcid.org/0000-0002-0640-0422
X-ray emission spectroscopy where the energy spectrum of the X-rays emitted due to core-to-core transitions is measured using a semiconductor detector.
FIX:0000104
FIX:0000677
EDAX
EDCS
EDS
EDS analysis
EDX
EDX analysis
EDXA
EDXRF
X-ray energy dispersive spectroscopy
X-ray energy-dispersive spectroscopy
energy dispersive X-ray (EDX) analysis
energy dispersive X-ray analysis
energy dispersive X-ray emission spectroscopy
energy dispersive X-ray fluorescence spectrometry
energy dispersive X-ray fluorescence spectroscopy
energy dispersive X-ray spectrometry
energy dispersive X-ray spectroscopy
energy dispersive spectroscopy
energy distribution curve spectroscopy
energy distribution spectroscopy
energy-dispersive X-ray emission analysis
energy-dispersive spectrometry
CHMO:0000309
energy-dispersive X-ray emission spectroscopy
X-ray emission spectroscopy where the energy spectrum of the X-rays emitted due to core-to-core transitions is measured using a semiconductor detector.
OrangeBook:16.2
X-ray spectroscopy where the sample is bombarded with incident X-rays of a wavelength which does not correspond to a specific electronic transition within the atoms of the sample, and the energies and intensities of the emitted X-rays are measured.
NRIXS
NRXES
NXES
non-resonant X-ray emission spectrometry
CHMO:0000310
non-resonant X-ray emission spectroscopy
X-ray spectroscopy where the sample is bombarded with incident X-rays of a wavelength which does not correspond to a specific electronic transition within the atoms of the sample, and the energies and intensities of the emitted X-rays are measured.
https://orcid.org/0000-0002-0640-0422
X-ray emission spectroscopy where the X-rays are generated by bombarding the sample with a focused beam of high-energy particles.
PIXE
PIXES
particle-induced X-ray emission spectrometry
CHMO:0000311
particle-induced X-ray emission spectroscopy
X-ray emission spectroscopy where the X-rays are generated by bombarding the sample with a focused beam of high-energy particles.
FIX:0000101
https://orcid.org/0000-0002-0640-0422
X-ray emission spectroscopy where the X-rays are generated by bombarding the sample with a finely focused (<10 m diameter) beam of high-energy particles.
PIXE microanalysis
microbeam PIXE
CHMO:0000312
microbeam particle-induced X-ray emission spectroscopy
X-ray emission spectroscopy where the X-rays are generated by bombarding the sample with a finely focused (<10 m diameter) beam of high-energy particles.
https://orcid.org/0000-0002-0640-0422
X-ray emission spectroscopy where the X-rays are generated by bombarding a flat polished sample with a finely focused (<10 μm diameter) beam of electrons which results in the ionisation of the inner shells of sample atoms. The decay of the ionised states results in the emission of characteristic X-rays.
FIX:0000105
FIX:0000674
EMPA
EPMA
EPXMA
electron micro-probe analysis
electron microprobe analysis
electron probe microanalysis
CHMO:0000313
electron probe X-ray microanalysis
X-ray emission spectroscopy where the X-rays are generated by bombarding a flat polished sample with a finely focused (<10 μm diameter) beam of electrons which results in the ionisation of the inner shells of sample atoms. The decay of the ionised states results in the emission of characteristic X-rays.
https://orcid.org/0000-0002-0640-0422
X-ray emission spectroscopy where the energy spectrum of the X-rays emitted due to core-to-core transitions is measured using a diffraction grating or crystal.
WD-XRF
WDS
WDX
WDXRF
wavelength dispersive X-ray emission spectrometry
wavelength dispersive X-ray fluorescence spectrometry
wavelength dispersive X-ray fluorescence spectroscopy
wavelength dispersive X-ray spectrometry
wavelength dispersive X-ray spectroscopy
CHMO:0000314
wavelength dispersive X-ray spectroscopy
X-ray emission spectroscopy where the energy spectrum of the X-rays emitted due to core-to-core transitions is measured using a diffraction grating or crystal.
Orange:16.2
X-ray spectroscopy where the sample is bombarded with a finely focused (<10 m diameter) X-ray beam and the energies and intensities of the X-rays emitted due to core-to-core transitions (known as 'X-ray fluorescence') are detected.
X-ray microemission
X-ray microemission spectrometry
X-ray microemission spectroscopy
X-ray microfluorescence
X-ray microfluorescence spectrometry
X-ray microfluorescence spectroscopy
XRME
XRME spectrometry
XRME spectroscopy
XRMF
XRMF spectrometry
XRMF spectroscopy
CHMO:0000315
X-ray microemission spectroscopy
X-ray spectroscopy where the sample is bombarded with a finely focused (<10 m diameter) X-ray beam and the energies and intensities of the X-rays emitted due to core-to-core transitions (known as 'X-ray fluorescence') are detected.
https://orcid.org/0000-0002-0640-0422
X-ray spectroscopy where the sample is bombarded with low energy X-rays and the energies and intensities of the X-rays emitted due to valence-to-core transitions are detected.
FIX:0000672
SXES
VBXES
soft X-ray emission spectrometry
soft X-ray fluorescence spectrometry
soft X-ray fluorescence spectroscopy
valence band X-ray emission spectrometry
valence band X-ray emission spectroscopy
valence band X-ray fluorescence spectrometry
valence band X-ray fluorescence spectroscopy
valence to core X-ray emission spectrometry
valence to core X-ray emission spectroscopy
valence to core X-ray fluorescence spectrometry
valence to core X-ray fluorescence spectroscopy
valence to core XES
valence to core XFS
valence-to-core X-ray emission spectrometry
valence-to-core X-ray emission spectroscopy
valence-to-core X-ray fluorescence spectrometry
valence-to-core X-ray fluorescence spectroscopy
valence-to-core XES
valence-to-core XFS
CHMO:0000316
soft X-ray emission spectroscopy
X-ray spectroscopy where the sample is bombarded with low energy X-rays and the energies and intensities of the X-rays emitted due to valence-to-core transitions are detected.
OrangeBook:17.2.2.2
X-ray spectroscopy where the sample is bombarded with ultra-low energy (<1 keV) X-rays and the energies and intensities of the X-rays emitted due to valence-to-core transitions are detected.
USX
USX spectrometry
USX spectroscopy
USXES
USXS
ultra soft X-ray emission spectrometry
ultra soft X-ray fluorescence spectrometry
ultra soft X-ray fluorescence spectroscopy
ultra-soft X-ray emission spectrometry
ultra-soft X-ray fluorescence spectrometry
ultra-soft X-ray fluorescence spectroscopy
CHMO:0000317
ultra soft X-ray emission spectroscopy
X-ray spectroscopy where the sample is bombarded with ultra-low energy (<1 keV) X-rays and the energies and intensities of the X-rays emitted due to valence-to-core transitions are detected.
10.1051/jphyscol:19879119
X-ray spectroscopy where the sample is bombarded with radiation is generated in a synchrotron and the energies and intensities of the emitted X-rays are detected.
synchrotron radiation excited X-ray spectrometry
CHMO:0000318
synchrotron radiation excited X-ray spectroscopy
X-ray spectroscopy where the sample is bombarded with radiation is generated in a synchrotron and the energies and intensities of the emitted X-rays are detected.
https://orcid.org/0000-0002-0640-0422
Spectroscopy where the sample is bombarded with X-rays and the energies of reflected X-rays are measured.
X-ray reflection spectrometry
X-ray reflectivity spectrometry
X-ray reflectivity spectroscopy
CHMO:0000319
X-ray reflection spectroscopy
Spectroscopy where the sample is bombarded with X-rays and the energies of reflected X-rays are measured.
https://orcid.org/0000-0002-0640-0422
Spectroscopy where the sample is bombarded with X-rays and the energies of totally reflected X-rays are measured.
TXRF
total reflection X-ray fluorescence analysis
total reflection X-ray fluorescence spectrometry
CHMO:0000320
total reflection X-ray fluorescence spectroscopy
Spectroscopy where the sample is bombarded with X-rays and the energies of totally reflected X-rays are measured.
https://orcid.org/0000-0002-0640-0422
Spectroscopy where the beta-particles spontaneously emitted from radioisotopes are detected.
beta spectrometry
beta spectroscopy
beta-particle spectrometry
CHMO:0000321
beta-particle spectroscopy
Spectroscopy where the beta-particles spontaneously emitted from radioisotopes are detected.
ISBN:0-19-280031-0
Spectroscopy where the spontaneous emission of a beta-particle produces a flash of light (known as a 'scintillation') which is detected.
CHMO:0000322
liquid scintillation counting
Spectroscopy where the spontaneous emission of a beta-particle produces a flash of light (known as a 'scintillation') which is detected.
ISBN:0-19-280102-3
Spectroscopy based on the differential absorption of left- and right-handed circularly polarised light by a sample.
CD spectrometry
CD spectroscopy
circular dichrosim spectrometry
direct transmittance circular dichroism
CHMO:0000323
circular dichroism spectroscopy
Spectroscopy based on the differential absorption of left- and right-handed circularly polarised light by a sample.
FIX:0000043
ISBN:0-19-280031-0
Spectroscopy based on the differential absorption of left- and right-handed circularly polarised luminescence.
FDCD
FDCD spectrometry
FDCD spectroscopy
fluorescence detected circular dichroism spectrometry
CHMO:0000324
fluorescence detected circular dichroism spectroscopy
Spectroscopy based on the differential absorption of left- and right-handed circularly polarised luminescence.
https://doi.org/10.1039/b504421a
Spectroscopy based on the differential absorption of left- and right-handed circularly polarised photon radiation in the presence of a magnetic field.
MCD
MCD spectrometry
MCD spectroscopy
magnetic circular dichroism spectrometry
CHMO:0000325
magnetic circular dichroism spectroscopy
Spectroscopy based on the differential absorption of left- and right-handed circularly polarised photon radiation in the presence of a magnetic field.
FIX:0000044
https://orcid.org/0000-0002-0640-0422
Spectroscopy based on the differential absorption of left- and right-handed circularly polarised X-ray radiation in the presence of a magnetic field.
X-ray magnetic circular dichroism spectrometry
XMCD
XMCD spectrometry
XMCD spectroscopy
CHMO:0000326
X-ray magnetic circular dichroism spectroscopy
Spectroscopy based on the differential absorption of left- and right-handed circularly polarised X-ray radiation in the presence of a magnetic field.
FIX:0001136
https://orcid.org/0000-0002-0640-0422
Spectroscopy based on the differential absorption of left- and right-handed circularly polarised infrared radiation during a vibrational transition.
VCD
VCD spectrometry
VCD spectroscopy
vibrating circular dichroism spectrometry
vibrational CD
vibrational circular dichroism
CHMO:0000327
vibrational circular dichroism spectroscopy
Spectroscopy based on the differential absorption of left- and right-handed circularly polarised infrared radiation during a vibrational transition.
FIX:0000231
ISBN:0471330035
Spectroscopy where the response of an atom with an unpaired electron to a perturbing magnetic field is measured.
EPR
EPR spectroscopy
ESR
ESR spectroscopy
electron paramagnetic resonance spectrometry
electron paramagnetic resonance spectroscopy
electron spin resonance spectrometry
CHMO:0000328
electron spin resonance spectroscopy
Spectroscopy where the response of an atom with an unpaired electron to a perturbing magnetic field is measured.
FIX:0000023
https://orcid.org/0000-0002-0640-0422
Spectroscopy where the response of an atom with an unpaired electron to a perturbing magnetic field is measured as a function of the frequency of a periodic perturbation.
FIX:0000033
c.w. EPR
c.w. ESR
continuous wave EPR
continuous wave ESR
continuous wave electron paramagnetic resonance spectroscopy
continuous wave electron spin resonance spectrometry
continuous wave electron spin resonance spectroscopy
cw-EPR
cw-ESR
CHMO:0000329
continuous-wave electron spin resonance spectroscopy
Spectroscopy where the response of an atom with an unpaired electron to a perturbing magnetic field is measured as a function of the frequency of a periodic perturbation.
ISBN:9780137217625
Spectroscopy where the response of an atom with an unpaired electron to short (ns) pulses of microwave radiation in a magnetic field is measured.
FIX:0000034
pulse EPR
pulse ESR
pulse electron paramagnetic resonance spectroscopy
pulse electron spin resonance spectrometry
pulsed EPR
pulsed ESR
pulsed electron spin resonance spectroscopy
CHMO:0000330
pulsed electron spin resonance spectroscopy
Spectroscopy where the response of an atom with an unpaired electron to short (ns) pulses of microwave radiation in a magnetic field is measured.
https://orcid.org/0000-0002-0640-0422
Spectroscopy where the absorption or emission of electrons is detected.
ES
electron spectrometry
CHMO:0000331
electron spectroscopy
Spectroscopy where the absorption or emission of electrons is detected.
FIX:0000064
OrangeBook:17.2
Spectroscopy where the sample is bombarded with an electron beam and the energy threshold for excitation is indicated by the appearance of relaxation products (Auger electrons or X-rays) or by a change in the electron beam current.
APS
appearance potential spectrometry
CHMO:0000332
appearance potential spectroscopy
Spectroscopy where the sample is bombarded with an electron beam and the energy threshold for excitation is indicated by the appearance of relaxation products (Auger electrons or X-rays) or by a change in the electron beam current.
OrangeBook:17.2.3
Spectroscopy where the sample is bombarded with an electron beam and the energy threshold for excitation is indicated by a sudden increase in secondary electron current.
AEAPS
Auger electron appearance potential spectrometry
EAAPS
IEMM
electron-excited Auger electron appearance potential spectrometry
electron-excited Auger electron appearance potential spectroscopy
incident energy modulation method spectrometry
incident energy modulation method spectroscopy
CHMO:0000333
Auger electron appearance potential spectroscopy
Spectroscopy where the sample is bombarded with an electron beam and the energy threshold for excitation is indicated by a sudden increase in secondary electron current.
OrangeBook:17.2.3
Spectroscopy where the sample is bombarded with an electron beam and the energy threshold for excitation is indicated by the sudden disappearance of electrons from the beam.
DAPS
disappearance potential spectrometry
CHMO:0000334
disappearance potential spectroscopy
Spectroscopy where the sample is bombarded with an electron beam and the energy threshold for excitation is indicated by the sudden disappearance of electrons from the beam.
Orange:17.2.3
Spectroscopy where the sample is bombarded with an electron beam and the energy threshold for excitation is indicated by a sudden change in the electron beam current. The fine structure close to the threshold is analysed by measuring the change in electron beam current.
EAPFS
EAPFSS
electron appearance potential fine structure spectrometry
electron appearance potential fine structure spectroscopy
extended appearance potential fine structure analysis
extended appearance potential fine structure spectrometry
extended appearance potential fine structure spectroscopy
CHMO:0000335
electron appearance potential fine structure analysis
Spectroscopy where the sample is bombarded with an electron beam and the energy threshold for excitation is indicated by a sudden change in the electron beam current. The fine structure close to the threshold is analysed by measuring the change in electron beam current.
Orange:17.2.3
Spectroscopy where the sample is bombarded with an electron beam and the energy threshold for excitation is determined by measuring the total electron current incident on the sample target.
TCS
target current spectrometry
target current spectroscopy
total current spectrometry
CHMO:0000336
total current spectroscopy
Spectroscopy where the sample is bombarded with an electron beam and the energy threshold for excitation is determined by measuring the total electron current incident on the sample target.
Orange:17.2.3
Spectroscopy where the sample is bombarded with an electron beam and the energy threshold for excitation is indicated by the sudden appearance of soft X-ray fluorescence.
EEXAPS
EXAPS
SXAPS
X-ray appearance potential spectrometry
XAPS
electron-excited X-ray appearance potential spectrometry
electron-excited X-ray appearance potential spectroscopy
soft X-ray appearance potential spectrometry
soft X-ray appearance potential spectroscopy
CHMO:0000337
X-ray appearance potential spectroscopy
Spectroscopy where the sample is bombarded with an electron beam and the energy threshold for excitation is indicated by the sudden appearance of soft X-ray fluorescence.
Orange:17.2.3
Spectroscopy where the sample is bombarded with an electron beam and the energy threshold for excitation is indicated by the sudden appearance of peaks in the photoelectron spectrum.
X-ray excited electron appearance potential spectrometry
XEAPS
CHMO:0000338
X-ray excited electron appearance potential spectroscopy
Spectroscopy where the sample is bombarded with an electron beam and the energy threshold for excitation is indicated by the sudden appearance of peaks in the photoelectron spectrum.
Orange:17.2.3
Spectroscopy where a high energy photon ionises a core electron and an electron from a higher energy level descends to take its place, releasing sufficient energy to eject a second so-called 'Auger' electron and the energy of the Auger electron is detected as a function of incident photon energy.
AEES
Auger electron emission spectroscopy
Auger electron spectrometry
Auger spectrometry
Auger spectroscopy
AES
CHMO:0000339
Auger electron spectroscopy
Spectroscopy where a high energy photon ionises a core electron and an electron from a higher energy level descends to take its place, releasing sufficient energy to eject a second so-called 'Auger' electron and the energy of the Auger electron is detected as a function of incident photon energy.
ISBN:0-471-96523-5
AES
Spectroscopy where bombardment of a sample with high-energy photons results in the ionisation of core electrons and the emission of so-called 'Auger' electrons. The energies of these Auger electrons are detected as a function of emission angle.
ADAS
ARAES
angle-resolved Auger electron spectrometry
angle-resolved Auger electron spectroscopy
angular dependent Auger spectrometry
CHMO:0000340
angular dependent Auger electron spectroscopy
Spectroscopy where bombardment of a sample with high-energy photons results in the ionisation of core electrons and the emission of so-called 'Auger' electrons. The energies of these Auger electrons are detected as a function of emission angle.
https://orcid.org/0000-0002-0640-0422
Spectroscopy where bombardment of a sample with high-energy photons results in the ionisation of core electrons and the emission of so-called 'Auger' electrons. The wavelength of the incident photons is scanned over an absorption edge in the sample and the Auger electrons emitted are detected as a function of energy.
RAES
resonance AES
resonance Auger electron spectrometry
resonance Auger electron spectroscopy
resonance Auger spectrometry
resonance Auger spectroscopy
resonant AES
resonant Auger electron spectrometry
resonant Auger spectrometry
resonant Auger spectroscopy
CHMO:0000341
resonant Auger electron spectroscopy
Spectroscopy where bombardment of a sample with high-energy photons results in the ionisation of core electrons and the emission of so-called 'Auger' electrons. The wavelength of the incident photons is scanned over an absorption edge in the sample and the Auger electrons emitted are detected as a function of energy.
https://doi.org/10.1103/PhysRevLett.88.243001
Spectroscopy where bombardment of a sample with high-energy photons results in the ionisation of core electrons and the emission of so-called 'Auger' electrons. The wavelength of the incident photons is scanned over an absorption edge in the sample and the Auger electrons emitted are detected as a function of emission angle.
angle-resolved resonance Auger electron spectrometry
angle-resolved resonance Auger electron spectroscopy
angle-resolved resonant Auger electron spectrometry
CHMO:0000342
angle-resolved resonant Auger electron spectroscopy
Spectroscopy where bombardment of a sample with high-energy photons results in the ionisation of core electrons and the emission of so-called 'Auger' electrons. The wavelength of the incident photons is scanned over an absorption edge in the sample and the Auger electrons emitted are detected as a function of emission angle.
https://orcid.org/0000-0002-0640-0422
Spectroscopy where bombardment of a sample with high-energy photons results in the ionisation of core electrons and the emission of so-called 'Auger' electrons. Only the Auger electrons emitted at a particular photon energy are detected.
APYS
Auger electron partial yield spectrometry
CHMO:0000343
Auger electron partial yield spectroscopy
Spectroscopy where bombardment of a sample with high-energy photons results in the ionisation of core electrons and the emission of so-called 'Auger' electrons. Only the Auger electrons emitted at a particular photon energy are detected.
OrangeBook:17.2.1.4
Spectroscopy where electron bombardment of a sample results in the ionisation of core electrons and the emission of so-called 'Auger' electron and the energies of these Auger electrons are detected as a function of incident electron energy.
EAES
EEAES
EIAES
electron-excited Auger electron spectrometry
electron-induced Auger electron spectrometry
electron-induced Auger electron spectroscopy
CHMO:0000344
electron-excited Auger electron spectroscopy
Spectroscopy where electron bombardment of a sample results in the ionisation of core electrons and the emission of so-called 'Auger' electron and the energies of these Auger electrons are detected as a function of incident electron energy.
Orange:17.2.4
Spectroscopy where bombardment of a sample with a finely focused (<10 m diameter) beam of electrons results in the ionisation of core electrons and the emission of so-called 'Auger' electrons. The energies of these Auger electrons are detected as a function of incident electron energy.
Auger electron microanalysis
EMAS
electron microprobe Auger electron spectrometry
CHMO:0000345
electron microprobe Auger spectroscopy
Spectroscopy where bombardment of a sample with a finely focused (<10 m diameter) beam of electrons results in the ionisation of core electrons and the emission of so-called 'Auger' electrons. The energies of these Auger electrons are detected as a function of incident electron energy.
https://orcid.org/0000-0002-0640-0422
Spectroscopy where ion bombardment of a sample results in the ionisation of core electrons and the emission of so-called 'Auger' electrons, which are detected as a function of incident ion energy.
IAES
IEAES
IIAES
ion neutralisation spectrometry
ion neutralisation spectroscopy
ion neutralization spectrometry
ion neutralization spectroscopy
ion-electron spectroscopy
ion-excited Auger spectrometry
ion-induced Auger electron spectrometry
ion-induced Auger electron spectroscopy
ionelectron spectroscopy
INS
CHMO:0000346
ion-excited Auger electron spectroscopy
Spectroscopy where ion bombardment of a sample results in the ionisation of core electrons and the emission of so-called 'Auger' electrons, which are detected as a function of incident ion energy.
Orange:17.2.4
Spectroscopy where the bombardment of a sample with He+ ions results in the ionisation of core electrons and the emission of so-called 'Auger' electrons, which are detected as a function of incident He+ ion energy.
HAES
He+-excited Auger electron spectrometry
CHMO:0000347
He+-excited Auger electron spectroscopy
Spectroscopy where the bombardment of a sample with He+ ions results in the ionisation of core electrons and the emission of so-called 'Auger' electrons, which are detected as a function of incident He+ ion energy.
https://orcid.org/0000-0002-0640-0422
Spectroscopy where the bombardment of a sample with protons results in the ionisation of core electrons and the emission of so-called 'Auger' electrons, which are detected as a function of incident proton energy.
PAES
proton-induced Auger electron spectrometry
CHMO:0000348
proton-induced Auger electron spectroscopy
Spectroscopy where the bombardment of a sample with protons results in the ionisation of core electrons and the emission of so-called 'Auger' electrons, which are detected as a function of incident proton energy.
https://orcid.org/0000-0002-0640-0422
Spectroscopy where ion bombardment of a sample results in the ionisation of core electrons and the emission of so-called 'Auger' electrons, which are detected as a function of emission angle.
AIRES
angle-resolved ion-electron spectrometry
angle-resolved ion-electron spectroscopy
CHMO:0000349
angle-resolved ion-excited Auger electron spectroscopy
Spectroscopy where ion bombardment of a sample results in the ionisation of core electrons and the emission of so-called 'Auger' electrons, which are detected as a function of emission angle.
https://orcid.org/0000-0002-0640-0422
Spectroscopy where a high-energy photon beam is scanned over the surface of a sample resulting in the ionisation of core electrons and the emission of so-called 'Auger' electrons. The energies of these Auger electrons are detected as a function of incident photon energy.
SAES
scanning Auger electron spectrometry
scanning Auger spectrometry
scanning Auger spectroscopy
CHMO:0000350
scanning Auger electron spectroscopy
Spectroscopy where a high-energy photon beam is scanned over the surface of a sample resulting in the ionisation of core electrons and the emission of so-called 'Auger' electrons. The energies of these Auger electrons are detected as a function of incident photon energy.
https://orcid.org/0000-0002-0640-0422
Spectroscopy where the bombardment of a sample with high-energy photons results in the ionisation of core electrons and the emission of so-called 'Auger' electrons. The energies of these Auger electrons are detected as a function of incident photon energy and a magnet is used to align all electron spins parallel to the emitting surface.
SPAES
spin-polarized Auger electron spectrometry
CHMO:0000351
spin-polarised Auger electron spectroscopy
Spectroscopy where the bombardment of a sample with high-energy photons results in the ionisation of core electrons and the emission of so-called 'Auger' electrons. The energies of these Auger electrons are detected as a function of incident photon energy and a magnet is used to align all electron spins parallel to the emitting surface.
OrangeBook:17.2.4
Spectroscopy where the bombardment of a sample with high-energy photons results in the ionisation of core electrons and the emission of so-called 'Auger' electrons. The energies of these Auger electrons are detected as a function of emission angle and a magnet is used to align all electron spins parallel to the emitting surface.
SPARPES
spin-polarized angle-resolved Auger electron spectrometry
CHMO:0000352
spin-polarised angle-resolved Auger electron spectroscopy
Spectroscopy where the bombardment of a sample with high-energy photons results in the ionisation of core electrons and the emission of so-called 'Auger' electrons. The energies of these Auger electrons are detected as a function of emission angle and a magnet is used to align all electron spins parallel to the emitting surface.
https://orcid.org/0000-0002-0640-0422
Spectroscopy where X-ray bombardment of a sample results in the ionisation of core electrons and the emission of so-called 'Auger' electrons, which are detected as a function of incident X-ray energy.
X-ray excited Auger electron spectrometry
X-ray induced Auger electron spectrometry
X-ray induced Auger electron spectroscopy
XAES
XEAES
XIAES
CHMO:0000353
X-ray excited Auger electron spectroscopy
Spectroscopy where X-ray bombardment of a sample results in the ionisation of core electrons and the emission of so-called 'Auger' electrons, which are detected as a function of incident X-ray energy.
Orange:17.2.4
Spectroscopy where the bombardment of a sample with a continuous X-ray source (X-rays generated when electrons, or other high energy charged particles such as protons or alpha-particles, lose energy whilst passing through the Coulomb field of a nucleus) results in the ionisation of core electrons and the emission of so-called 'Auger' electrons, which are detected.
CX-AES
CXAES
bremsstrahlung Auger electron spectrometry
bremsstrahlung Auger electron spectroscopy
bremsstrahlung Auger spectrometry
bremsstrahlung Auger spectroscopy
continuous X-ray-induced Auger electron spectrometry
continuous X-ray-induced Auger spectrometry
continuous X-ray-induced Auger spectroscopy
CHMO:0000354
continuous X-ray-induced Auger electron spectroscopy
Spectroscopy where the bombardment of a sample with a continuous X-ray source (X-rays generated when electrons, or other high energy charged particles such as protons or alpha-particles, lose energy whilst passing through the Coulomb field of a nucleus) results in the ionisation of core electrons and the emission of so-called 'Auger' electrons, which are detected.
ISBN:0824706005
Spectroscopy where two or more particles (electrons, photons or ions) originating from a single event, such as an ionisation, are detected as a function of energy.
ECS
electron coincidence spectrometry
CHMO:0000355
electron coincidence spectroscopy
Spectroscopy where two or more particles (electrons, photons or ions) originating from a single event, such as an ionisation, are detected as a function of energy.
Orange:17.2.5
Spectroscopy where the sample is bombarded with X-rays resulting in the emission of photoelectrons and 'Auger' electrons which are detected as a function of energy.
AEPECS
APECS
Auger electron photoelectron coincidence spectrometry
Auger electron-photoelectron coincidence spectroscopy
Auger-photoelectron electron coincidence spectrometry
CHMO:0000356
Auger-photoelectron coincidence spectroscopy
Spectroscopy where the sample is bombarded with X-rays resulting in the emission of photoelectrons and 'Auger' electrons which are detected as a function of energy.
https://orcid.org/0000-0002-0640-0422
Spectroscopy where the sample is bombarded with high-energy photons resulting in the emission of a pair of electrons which are detected as a function of energy.
E2E
electron-electron coincidence spectrometry
CHMO:0000357
electron-electron coincidence spectroscopy
Spectroscopy where the sample is bombarded with high-energy photons resulting in the emission of a pair of electrons which are detected as a function of energy.
https://orcid.org/0000-0002-0640-0422
Spectroscopy where the sample is bombarded with high-energy photons resulting in the emission of a pair of electrons which are detected as a function of emission angle.
ARE2E
angle-resolved E2E
angle-resolved electron-electron coincidence spectrometry
CHMO:0000358
angle-resolved electron-electron coincidence spectroscopy
Spectroscopy where the sample is bombarded with high-energy photons resulting in the emission of a pair of electrons which are detected as a function of emission angle.
https://orcid.org/0000-0002-0640-0422
Spectroscopy where the sample is bombarded with high-energy photons resulting in the emission of an ion and a pair of electrons which are detected as a function of energy.
EEICO
electron-electron ion coincidence spectrometry
CHMO:0000359
electron-electron-ion coincidence spectroscopy
Spectroscopy where the sample is bombarded with high-energy photons resulting in the emission of an ion and a pair of electrons which are detected as a function of energy.
https://orcid.org/0000-0002-0640-0422
Spectroscopy where the sample is bombarded with high-energy photons resulting in the emission of an ion and a pair of electrons which are detected as a function of emission angle.
AREEICO
angle-resolved electron-electron ion coincidence spectrometry
CHMO:0000360
angle-resolved electron-electron ion coincidence spectroscopy
Spectroscopy where the sample is bombarded with high-energy photons resulting in the emission of an ion and a pair of electrons which are detected as a function of emission angle.
https://orcid.org/0000-0002-0640-0422
Spectroscopy where the sample is bombarded with high-energy photons resulting in the emission of an ion and an electron which are detected as a function of energy.
EICO
electron-ion coincidence spectrometry
CHMO:0000361
electron-ion coincidence spectroscopy
Spectroscopy where the sample is bombarded with high-energy photons resulting in the emission of an ion and an electron which are detected as a function of energy.
https://orcid.org/0000-0002-0640-0422
Spectroscopy where the sample is bombarded with metastable atoms resulting in the emission of two or more particles (electrons, photons or ions) which are detected as a function of energy.
MQES
metastable-quenched electron spectrometry
CHMO:0000362
metastable-quenched electron spectroscopy
Spectroscopy where the sample is bombarded with metastable atoms resulting in the emission of two or more particles (electrons, photons or ions) which are detected as a function of energy.
Orange:17.2.6
Spectroscopy where the sample is bombarded with metastable atoms resulting in the emission of an electron (by resonant ionisation) and an Auger electron.
RIS
resonance-ionisation spectrometry
resonance-ionization spectrometry
resonance-ionization spectroscopy
CHMO:0000363
resonance-ionisation spectroscopy
Spectroscopy where the sample is bombarded with metastable atoms resulting in the emission of an electron (by resonant ionisation) and an Auger electron.
Orange:17.2.6
Spectroscopy where the sample is bombarded with metastable atoms resulting in the emission of an electron (by Penning ionisation) and an Auger electron.
SPIES
surface Penning-ionisation electron spectrometry
surface Penning-ionization electron spectrometry
surface Penning-ionization electron spectroscopy
CHMO:0000364
surface Penning-ionisation electron spectroscopy
Spectroscopy where the sample is bombarded with metastable atoms resulting in the emission of an electron (by Penning ionisation) and an Auger electron.
Orange:17.2.6
Spectroscopy where the sample is bombarded with high-energy photons resulting in the emission of a photoelectron and its corresponding ion which are detected as a function of energy.
PIPECO
photoion photoelectron coincidence spectrometry
photoion photoelectron coincidence spectroscopy
photoion-photoelectron coincidence spectrometry
photoionphotoelectron coincidence spectrometry
photoionphotoelectron coincidence spectroscopy
CHMO:0000365
photoion-photoelectron coincidence spectroscopy
Spectroscopy where the sample is bombarded with high-energy photons resulting in the emission of a photoelectron and its corresponding ion which are detected as a function of energy.
https://doi.org/a909621c
Spectroscopy where a beam of electrons with a known, narrow range of kinetic energies (50–200 eV) interacts with a surface and the energy loss (0.005–100 eV) the electrons suffer as a result of the interaction is measured.
EELS
IESS
REELS
electron energy loss spectrometry
electron impact spectroscopy
inelastic electron scattering spectrometry
inelastic electron scattering spectroscopy
reflection electron energy loss spectrometry
reflection electron energy loss spectroscopy
EIS
ELS
CHMO:0000366
electron energy loss spectroscopy
Spectroscopy where a beam of electrons with a known, narrow range of kinetic energies (50–200 eV) interacts with a surface and the energy loss (0.005–100 eV) the electrons suffer as a result of the interaction is measured.
FIX:0000663
FIX:0000664
ISBN:0-19-280031-0
https://doi.org/10.1351/goldbook.R05236
Spectroscopy where a beam of electrons with a known, narrow range of kinetic energies is reflected by a surface and the number of electrons with a given characteristic energy loss is measured.
CELS
characteristic energy loss spectrometry
characteristic energy loss spectroscopy
characteristic energy-loss spectrometry
CHMO:0000367
characteristic energy-loss spectroscopy
Spectroscopy where a beam of electrons with a known, narrow range of kinetic energies is reflected by a surface and the number of electrons with a given characteristic energy loss is measured.
ISBN:0387258000
Spectroscopy where a beam of electrons with a known, extended range of kinetic energies is reflected by a surface and the energy loss the electrons suffer upon reflection is measured. Measurements are taken from the absorption edge onset to several hundred eV above it.
EELFS
ELFS spectrometry
ELFS spectroscopy
EXEELFS
EXELFS spectrometry
EXELFS spectroscopy
extended electron energy loss fine structure spectrometry
extended energy loss fine structure spectrometry
extended energy loss fine structure spectroscopy
CHMO:0000368
extended electron energy loss fine structure spectroscopy
Spectroscopy where a beam of electrons with a known, extended range of kinetic energies is reflected by a surface and the energy loss the electrons suffer upon reflection is measured. Measurements are taken from the absorption edge onset to several hundred eV above it.
FIX:0000668
https://orcid.org/0000-0002-0640-0422
Spectroscopy where a beam of electrons with a known, extended range of kinetic energies is reflected by a surface and the Auger emission is measured. Measurements are taken from the absorption edge onset to several hundred eV above it.
EXFAS
SEELFS
extended fine Auger structures
CHMO:0000369
surface extended electron energy loss fine structure spectroscopy
Spectroscopy where a beam of electrons with a known, extended range of kinetic energies is reflected by a surface and the Auger emission is measured. Measurements are taken from the absorption edge onset to several hundred eV above it.
https://orcid.org/0000-0002-0640-0422
Spectroscopy where a beam of electrons with a known, narrow range of kinetic energies is reflected by a surface and the small energy loss (0.02–1 eV) the electrons suffer upon reflection is measured.
HEELS
HR-EELS
HREELS
HRELS
VELS
high resolution energy loss spectrometry
high resolution energy loss spectroscopy
high-resolution energy loss spectroscopy
vibrational ELS
vibrational energy loss spectroscopy
CHMO:0000370
high-resolution energy loss spectroscopy
Spectroscopy where a beam of electrons with a known, narrow range of kinetic energies is reflected by a surface and the small energy loss (0.02–1 eV) the electrons suffer upon reflection is measured.
FIX:0000646
https://doi.org/10.1351/goldbook.H02826
Spectroscopy where the loss in energy of electrons produced by ionisation is measured.
CLS
core level characteristic loss spectroscopy
core-level characteristic loss spectroscopy
ionisation loss spectrometry
ionisation loss spectroscopy
ionisation spectrometry
ionization loss spectrometry
ionization loss spectroscopy
ionization spectrometry
ionization spectroscopy
ILS
IS
CHMO:0000371
ionisation spectroscopy
Spectroscopy where the loss in energy of electrons produced by ionisation is measured.
FIX:0000670
OrangeBook:17.2.2.1
Spectroscopy where a beam of electrons with a known, narrow range of low kinetic energies is reflected by a surface and the energy loss the electrons suffer upon reflection is measured.
LEELS
low energy electron energy loss spectrometry
low-energy electron energy loss spectrometry
low-energy electron energy loss spectroscopy
CHMO:0000372
low-energy electron loss spectroscopy
Spectroscopy where a beam of electrons with a known, narrow range of low kinetic energies is reflected by a surface and the energy loss the electrons suffer upon reflection is measured.
https://orcid.org/0000-0002-0640-0422
Spectroscopy where a beam of electrons with a known, narrow range of kinetic energies is transmitted through a sample and the energy distribution of the transmitted electrons is measured.
CHMO:0002296
ETS
TEELS
electron transmission spectrometry
electron transmission spectroscopy
CHMO:0000373
transmission electron energy loss spectroscopy
Spectroscopy where a beam of electrons with a known, narrow range of kinetic energies is transmitted through a sample and the energy distribution of the transmitted electrons is measured.
https://doi.org/10.1351/goldbook.T06480
Spectroscopy where a beam of electrons with a known, narrow range of kinetic energies is reflected by a surface and energy loss the electrons suffer (corresponding to vibrational modes in the sample) is measured.
VEELS
vibrational electron energy loss spectrometry
CHMO:0000374
vibrational electron energy loss spectroscopy
Spectroscopy where a beam of electrons with a known, narrow range of kinetic energies is reflected by a surface and energy loss the electrons suffer (corresponding to vibrational modes in the sample) is measured.
https://orcid.org/0000-0002-0640-0422
Any type of electron spectroscopy where electrons are emitted from a cathode by application of an intense electric field.
FEED spectrometry
FEED spectroscopy
FES
field emission electron spectroscopy
field emission energy distribution spectrometry
field emission energy distribution spectroscopy FEEDS
CHMO:0000375
field-emission electron spectroscopy
Any type of electron spectroscopy where electrons are emitted from a cathode by application of an intense electric field.
Orange:17.2.7
Any type of electron spectroscopy where electrons are emitted from a cathode by application of an intense electric field and a magnet is used to align all electron spins parallel to the sample surface.
FEESP
field emission electron spin-polarization spectroscopy
field-emitted electron spin-polarization spectrometry
CHMO:0000376
field-emission electron spin-polarization spectroscopy
Any type of electron spectroscopy where electrons are emitted from a cathode by application of an intense electric field and a magnet is used to align all electron spins parallel to the sample surface.
https://orcid.org/0000-0002-0640-0422
Spectroscopy where the sample is bombarded with electrons and the photons emitted are detected.
IPES
IPS
inverse photoelectron spectrometry
inverse photoemission spectrometry
inverse photoemission spectroscopy
CHMO:0000377
inverse photoelectron spectroscopy
Spectroscopy where the sample is bombarded with electrons and the photons emitted are detected.
FIX:0000687
OrangeBook:17.2.2.2
Spectroscopy where the sample is bombarded with electrons which decay in unoccupied states emitting bremsstrahlung radiation.
BIS
bremsstrahlung isochromat spectrometry
bremsstrahlung spectrometry
bremsstrahlung spectroscopy
CHMO:0000378
bremsstrahlung isochromat spectroscopy
Spectroscopy where the sample is bombarded with electrons which decay in unoccupied states emitting bremsstrahlung radiation.
Orange:17.2.2.2
Spectroscopy where the sample is bombarded with electrons which decay in unoccupied states emitting bremsstrahlung radiation which is detected as a function of emission angle.
CHMO:0000379
angle-resolved bremsstrahlung isochromat spectroscopy
Spectroscopy where the sample is bombarded with electrons which decay in unoccupied states emitting bremsstrahlung radiation which is detected as a function of emission angle.
https://doi.org/10.1103/PhysRevB.29.3015
Spectroscopy where the sample is bombarded with electrons which decay in unoccupied states emitting bremsstrahlung radiation which is detected as a function of photon momentum.
FIX:0000688
BS
momentum-resolved bremsstrahlung spectrometry
CHMO:0000380
momentum-resolved bremsstrahlung spectroscopy
Spectroscopy where the sample is bombarded with electrons which decay in unoccupied states emitting bremsstrahlung radiation which is detected as a function of photon momentum.
OrangeBook:17.2.2.2
Spectroscopy where the sample is bombarded with electrons which decay in unoccupied states emitting bremsstrahlung radiation in the ultraviolet region.
UVBIS
ultra-violet bremsstrahlung isochromat spectrometry
ultra-violet bremsstrahlung isochromat spectroscopy
ultra-violet bremsstrahlung spectrometry
ultraviolet bremsstrahlung isochromat spectrometry
ultraviolet bremsstrahlung isochromat spectroscopy
ultraviolet bremsstrahlung spectrometry
ultraviolet bremsstrahlung spectroscopy
CHMO:0000381
ultraviolet bremsstrahlung isochromat spectroscopy
Spectroscopy where the sample is bombarded with electrons which decay in unoccupied states emitting bremsstrahlung radiation in the ultraviolet region.
https://orcid.org/0000-0002-0640-0422
Spectroscopy where the sample is bombarded with electrons which decay in unoccupied states emitting bremsstrahlung radiation in the X-ray region.
X-ray bremsstrahlung spectrometry
XBIS
CHMO:0000382
X-ray bremsstrahlung isochromat spectroscopy
Spectroscopy where the sample is bombarded with electrons which decay in unoccupied states emitting bremsstrahlung radiation in the X-ray region.
https://orcid.org/0000-0002-0640-0422
Spectroscopy where the sample is bombarded with electrons which decay in unoccupied states emitting bremsstrahlung radiation which is detected as a function of the vector k (where k is the difference between the wave vectors of the incident and scattered radiation).
KRIPES
KRIPS
k-resolved IPE spectrometry
k-resolved IPE spectroscopy
k-resolved inverse photoelectron spectrometry
k-resolved inverse photoemission spectrometry
k-resolved inverse photoemission spectroscopy
CHMO:0000383
k-resolved inverse photoelectron spectroscopy
Spectroscopy where the sample is bombarded with electrons which decay in unoccupied states emitting bremsstrahlung radiation which is detected as a function of the vector k (where k is the difference between the wave vectors of the incident and scattered radiation).
https://orcid.org/0000-0002-0640-0422
Spectroscopy where a magnetised ferromagnetic sample is bombarded with electrons of a specific spin polarisation which decay in unoccupied states emitting bremsstrahlung radiation.
SPIPES
spin-polarized inverse photoelectron spectrometry
CHMO:0000384
spin-polarised inverse photoelectron spectroscopy
Spectroscopy where a magnetised ferromagnetic sample is bombarded with electrons of a specific spin polarisation which decay in unoccupied states emitting bremsstrahlung radiation.
Orange:17.2.1.4
Spectroscopy where energy transfer from a metastable atom in close proximity to (~5 ) the sample gives rise to a characteristic ejected electron energy spectrum.
MDS
metastable de-excitation spectrometry
metastable deexcitation spectrometry
metastable deexcitation spectroscopy
CHMO:0000385
metastable de-excitation spectroscopy
Spectroscopy where energy transfer from a metastable atom in close proximity to (~5 ) the sample gives rise to a characteristic ejected electron energy spectrum.
https://orcid.org/0000-0002-0640-0422
Spectroscopy where energy transfer from a metastable atom in close proximity to (~5 ) the sample gives rise to a characteristic ejected electron energy spectrum. A magnet is used to align all the electron spins parallel to the surface.
SP-MDS
SPMDS
spin-polarized metastable de-excitation spectrometry
spin-polarized metastable de-excitation spectroscopy
spin-polarized metastable deexcitation spectrometry
spin-polarized metastable deexcitation spectroscopy
CHMO:0000386
spin-polarized metastable de-excitation spectroscopy
Spectroscopy where energy transfer from a metastable atom in close proximity to (~5 ) the sample gives rise to a characteristic ejected electron energy spectrum. A magnet is used to align all the electron spins parallel to the surface.
https://orcid.org/0000-0002-0640-0422
Spectroscopy where the sample is illuminated with photons causing ionisation and the emission of photoelectrons, the energies of which are measured. The energy of the incident photons is usually greater than the ionisation energy of the sample and the photoelectrons are emitted with the excess in the form of kinetic energy.
PES
photo emission spectrometry
photo emission spectroscopy
photoelectron emission spectroscopy
photoelectron spectrometry
photoemission spectrometry
photoemission spectroscopy
PS
CHMO:0000387
photoelectron spectroscopy
Spectroscopy where the sample is illuminated with photons causing ionisation and the emission of photoelectrons, the energies of which are measured. The energy of the incident photons is usually greater than the ionisation energy of the sample and the photoelectrons are emitted with the excess in the form of kinetic energy.
FIX:0000040
https://doi.org/10.1351/goldbook.P04609
Spectroscopy where the sample is illuminated with photons causing ionisation and the emission of photoelectrons which are detected as a function of emission angle.
ARP
ARPES
ARPS
angle-resolved photoelectron spectrometry
angle-resolved photoemission spectrometry
angle-resolved photoemission spectroscopy
CHMO:0000388
angle-resolved photoelectron spectroscopy
Spectroscopy where the sample is illuminated with photons causing ionisation and the emission of photoelectrons which are detected as a function of emission angle.
FIX:0000665
https://orcid.org/0000-0002-0640-0422
Spectroscopy where the sample is illuminated with gamma-rays causing ionisation and the emission of photoelectrons, the energies of which are measured.
DSPES
depth-selective photoelectron spectrometry
depth-selective photoemission spectrometry
gamma-ray photoelectron spectrometry
gamma-ray photoelectron spectroscopy
gamma-ray photoemission spectrometry
gamma-ray photoemission spectroscopy
CHMO:0000389
depth-selective photoelectron spectroscopy
Spectroscopy where the sample is illuminated with gamma-rays causing ionisation and the emission of photoelectrons, the energies of which are measured.
FIX:0000675
https://orcid.org/0000-0002-0640-0422
Spectroscopy where the sample is illuminated with photons causing ionisation and the emission of photoelectrons which are detected as a function of energy. The spectrum is recorded over an extended energy range, from the photon absorption edge onset to several hundred eV above it.
PEFS
PEFS spectrometry
PEFS spectroscopy
PEFSS
CHMO:0000390
photoelectron extended fine structure spectroscopy
Spectroscopy where the sample is illuminated with photons causing ionisation and the emission of photoelectrons which are detected as a function of energy. The spectrum is recorded over an extended energy range, from the photon absorption edge onset to several hundred eV above it.
https://orcid.org/0000-0002-0640-0422
Spectroscopy where the sample is illuminated with photons causing ionisation and the emission of photoelectrons which are detected as a function of emission angle. The spectrum is recorded over an extended energy range, from the photon absorption edge onset to several hundred eV above it.
ARPEFS
ARPEFSS
ARPES spectrometry
ARPES spectroscopy
angle-resolved photoelectron extended fine structure spectrometry
angle-resolved photoemission extended fine structure spectrometry
angle-resolved photoemission extended fine structure spectroscopy
CHMO:0000391
angle-resolved photoelectron extended fine structure spectroscopy
Spectroscopy where the sample is illuminated with photons causing ionisation and the emission of photoelectrons which are detected as a function of emission angle. The spectrum is recorded over an extended energy range, from the photon absorption edge onset to several hundred eV above it.
https://orcid.org/0000-0002-0640-0422
Spectroscopy where the sample is illuminated with a finely focused (<10 m) photon beam causing ionisation and the emission of photoelectrons, the energies of which are measured.
PEMS
PESM
photoelectron micro-spectrometry
photoelectron micro-spectroscopy
photoelectron microspectrometry
CHMO:0000392
photoelectron microspectroscopy
Spectroscopy where the sample is illuminated with a finely focused (<10 m) photon beam causing ionisation and the emission of photoelectrons, the energies of which are measured.
https://doi.org/10.1116/1.581237
Spectroscopy where the sample is illuminated with a finely focused (<10 m) extreme ultraviolet (10–121 nm) photon beam causing ionisation and the emission of photoelectrons, the energies of which are measured.
EUV photoelectron micro-spectroscopy
EUV photoelectron microspectroscopy
extreme ultra-violet photoelectron microspectroscopy
CHMO:0000393
extreme ultraviolet photoelectron microspectroscopy
Spectroscopy where the sample is illuminated with a finely focused (<10 m) extreme ultraviolet (10–121 nm) photon beam causing ionisation and the emission of photoelectrons, the energies of which are measured.
ISBN:1-55752-706-7
Spectroscopy where the sample is illuminated with radiation (X-ray–ultraviolet) generated in a synchrotron causing ionisation and the emission of photoelectrons, the energies of which are measured.
SRPES
SRPS
synchrotron radiation photoelectron spectrometry
CHMO:0000394
synchrotron radiation photoelectron spectroscopy
Spectroscopy where the sample is illuminated with radiation (X-ray–ultraviolet) generated in a synchrotron causing ionisation and the emission of photoelectrons, the energies of which are measured.
FIX:0000676
OrangeBook:17.2.1.4
Spectroscopy where the sample is illuminated with radiation (X-ray–ultraviolet) generated in a synchrotron causing ionisation and the emission of photoelectrons which are detected as a function of emission angle.
angle-resolved synchotron radiation photoelectron spectrometry
CHMO:0000395
angle-resolved synchotron radiation photoelectron spectroscopy
Spectroscopy where the sample is illuminated with radiation (X-ray–ultraviolet) generated in a synchrotron causing ionisation and the emission of photoelectrons which are detected as a function of emission angle.
Orange:17.2.1.4
Spectroscopy where the sample is illuminated with radiation (X-ray–ultraviolet) generated in a synchrotron causing ionisation and the emission of photoelectrons. The energy distribution of electrons which have been promoted to a specific conduction band is measured.
CFSS
constant final state spectroscopy
constant-final-state spectrometry
CHMO:0000396
constant-final-state spectroscopy
Spectroscopy where the sample is illuminated with radiation (X-ray–ultraviolet) generated in a synchrotron causing ionisation and the emission of photoelectrons. The energy distribution of electrons which have been promoted to a specific conduction band is measured.
FIX:0000681
OrangeBook:17.2.1.4
Spectroscopy where the sample is illuminated with radiation (X-ray–ultraviolet) generated in a synchrotron causing ionisation and the emission of photoelectrons. The energy distribution of electrons which have been promoted from a specific valence band is measured.
CISS
constant initial state spectroscopy
constant-initial-state spectrometry
CHMO:0000397
constant-initial-state spectroscopy
Spectroscopy where the sample is illuminated with radiation (X-ray–ultraviolet) generated in a synchrotron causing ionisation and the emission of photoelectrons. The energy distribution of electrons which have been promoted from a specific valence band is measured.
Orange:17.2.1.4
Spectroscopy where the sample is illuminated with radiation (X-ray–ultraviolet) generated in a synchrotron causing ionisation and the emission of photoelectrons. All photoelectrons emitted at a particular photon energy are detected.
PEYS
photoelectron yield spectrometry
total yield spectroscopy
CHMO:0000398
photoelectron yield spectroscopy
Spectroscopy where the sample is illuminated with radiation (X-ray–ultraviolet) generated in a synchrotron causing ionisation and the emission of photoelectrons. All photoelectrons emitted at a particular photon energy are detected.
FIX:0000678
OrangeBook:17.2.1.4
Spectroscopy where the sample is illuminated with radiation (X-ray–ultraviolet) generated in a synchrotron causing ionisation and the emission of photoelectrons. All of the photoelectrons emitted within a certain energy interval are detected.
PYS
partial photoyield spectroscopy
partial yield spectrometry
partial yield spectroscopy
CHMO:0000399
partial-yield spectroscopy
Spectroscopy where the sample is illuminated with radiation (X-ray–ultraviolet) generated in a synchrotron causing ionisation and the emission of photoelectrons. All of the photoelectrons emitted within a certain energy interval are detected.
FIX:0000679
OrangeBook:17.2.1.4
Spectroscopy where the sample is illuminated with radiation (X-ray–ultraviolet) generated in a synchrotron causing ionisation and the emission of photoelectrons. The energy of the incoming photons is adjusted such that it coincides with an electronic transition of the molecule.
REPS
resonance-enhanced photoelectron spectrometry
CHMO:0000400
resonance-enhanced photoelectron spectroscopy
Spectroscopy where the sample is illuminated with radiation (X-ray–ultraviolet) generated in a synchrotron causing ionisation and the emission of photoelectrons. The energy of the incoming photons is adjusted such that it coincides with an electronic transition of the molecule.
FIX:0000685
OrangeBook:17.2.1.4
Spectroscopy where the sample is illuminated with ultraviolet (10–400 nm) photons causing ionisation and the emission of photoelectrons, the energies of which are measured.
UPES
UPS
UVPES
UVPS
ultra-violet photoelectron spectrometry
ultra-violet photoelectron spectroscopy
ultra-violet photoemission spectroscopy ultra-violet photoemission spectrometry
ultraviolet photoelectron spectrometry
ultraviolet photoelectron spectroscopy
ultraviolet photoemission spectrometry
ultraviolet photoemission spectroscopy
CHMO:0000401
ultraviolet photoelectron spectroscopy
Spectroscopy where the sample is illuminated with ultraviolet (10–400 nm) photons causing ionisation and the emission of photoelectrons, the energies of which are measured.
FIX:0000042
https://doi.org/10.1351/goldbook.U06583
Spectroscopy where the sample is illuminated with ultraviolet (10–400 nm) photons causing ionisation and the emission of photoelectrons, which are detected as a function of emission angle.
UVAIUPES
UVAIUPS
UVARUPES
UVARUPS
angle-integrated ultra-violet photoelectron spectrometry
angle-integrated ultra-violet photoelectron spectroscopy
angle-integrated ultra-violet photoemission spectrometry
angle-integrated ultraviolet photoelectron spectrometry
angle-integrated ultraviolet photoelectron spectroscopy
angle-integrated ultraviolet photoemission spectrometry
angle-integrated ultraviolet photoemission spectroscopy
angle-resolved ultra-violet photoelectron spectrometry
angle-resolved ultra-violet photoelectron spectroscopy
angle-resolved ultra-violet photoemission spectrometry
angle-resolved ultra-violet photoemission spectroscopy
angle-resolved ultraviolet photoelectron spectrometry
angle-resolved ultraviolet photoemission spectrometry
angle-resolved ultraviolet photoemission spectroscopy
CHMO:0000402
angle-resolved ultraviolet photoelectron spectroscopy
Spectroscopy where the sample is illuminated with ultraviolet (10–400 nm) photons causing ionisation and the emission of photoelectrons, which are detected as a function of emission angle.
FIX:0000683
https://orcid.org/0000-0002-0640-0422
Spectroscopy where the sample is illuminated with vacuum ultraviolet (10–20 nm) photons causing ionisation and the emission of photoelectrons, the energies of which are measured.
VUVPES
VUVPS
vacuum ultra-violet photoelectron spectrometry
vacuum ultra-violet photoelectron spectroscopy
vacuum ultra-violet photoemission spectrometry
vacuum ultraviolet photoelectron spectroscopy
vacuum ultraviolet photoemission spectroscopy
CHMO:0000403
vacuum ultraviolet photoelectron spectroscopy
Spectroscopy where the sample is illuminated with vacuum ultraviolet (10–20 nm) photons causing ionisation and the emission of photoelectrons, the energies of which are measured.
https://orcid.org/0000-0002-0640-0422
Spectroscopy where the sample is illuminated with X-rays causing ionisation and the emission of photoelectrons, the energies of which are measured.
FIX:0000041
ESCA
PESIS
X-ray photoelectron emission spectroscopy
X-ray photoelectron scattering (XPS) spectroscopy
X-ray photoelectron scattering spectroscopy
X-ray photoelectron spectrometry
X-ray photoemission spectroscopy
XPES
XPS
electron spectrometry for chemical analysis
electron spectrometry for chemical applications
electron spectroscopy for chemical analysis
electron spectroscopy for chemical applications
photoelectron spectroscopy of the inner shell
CHMO:0000404
X-ray photoelectron spectroscopy
Spectroscopy where the sample is illuminated with X-rays causing ionisation and the emission of photoelectrons, the energies of which are measured.
https://doi.org/10.1351/goldbook.X06716
Spectroscopy where the sample is illuminated with X-rays causing ionisation and the emission of photoelectrons, which are detected as a function of emission angle.
ARXPS
angle-resolved X-ray photoelectron spectrometry
CHMO:0000405
angle-resolved X-ray photoelectron spectroscopy
Spectroscopy where the sample is illuminated with X-rays causing ionisation and the emission of photoelectrons, which are detected as a function of emission angle.
FIX:0000684
https://orcid.org/0000-0002-0640-0422
Spectroscopy where the sample is illuminated with monochromatic X-rays causing ionisation and the emission of photoelectrons, the energies of which are measured.
HR-XPS
HRXPS
high resolution X-ray photoelectron spectrometry
high resolution X-ray photoelectron spectroscopy
high resolution X-ray photoemission spectrometry
high resolution X-ray photoemission spectroscopy
high-resolution X-ray photoelectron spectrometry
high-resolution X-ray photoemission spectrometry
CHMO:0000406
high-resolution X-ray photoelectron spectroscopy
Spectroscopy where the sample is illuminated with monochromatic X-rays causing ionisation and the emission of photoelectrons, the energies of which are measured.
https://orcid.org/0000-0002-0640-0422
Spectroscopy where the sample is illuminated with 'soft' (<300 eV) X-rays causing ionisation and the emission of photoelectrons, the energies of which are measured.
SXPS
soft X-ray photoelectron spectrometry
CHMO:0000407
soft X-ray photoelectron spectroscopy
Spectroscopy where the sample is illuminated with 'soft' (<300 eV) X-rays causing ionisation and the emission of photoelectrons, the energies of which are measured.
Orange:17.2.1.2
Spectroscopy where the sample is illuminated with monochromatic 'soft' (<300 eV) X-rays causing ionisation and the emission of photoelectrons, the energies of which are measured.
HR-SXPS
HRSXPS
high resolution soft X-ray photoelectron spectrometry
high resolution soft X-ray photoelectron spectroscopy
high resolution soft X-ray photoemission spectrometry
high resolution soft X-ray photoemission spectroscopy
high-resolution soft X-ray photoelectron spectrometry
high-resolution soft X-ray photoemission spectrometry
CHMO:0000408
high-resolution soft X-ray photoelectron spectroscopy
Spectroscopy where the sample is illuminated with monochromatic 'soft' (<300 eV) X-rays causing ionisation and the emission of photoelectrons, the energies of which are measured.
https://doi.org/10.1107/S0909049502009214
Spectroscopy where the sample is illuminated with photons causing ionisation of the valence shell and the emission of photoelectrons, the energies of which are measured.
valence-shell photoionisation spectrometry
valence-shell photoionization spectrometry
CHMO:0000409
valence-shell photoionisation spectroscopy
Spectroscopy where the sample is illuminated with photons causing ionisation of the valence shell and the emission of photoelectrons, the energies of which are measured.
https://orcid.org/0000-0002-0640-0422
Spectroscopy where the sample is illuminated with photons causing ionisation and the emission of photoelectrons, the energies of which are measured. The energy of the incident photons matches the ionisation energy of the sample so emitted electrons have zero kinetic energy.
ZEKE spectrometry
zero kinetic energy electron spectrometry
CHMO:0000410
zero kinetic energy electron spectroscopy
Spectroscopy where the sample is illuminated with photons causing ionisation and the emission of photoelectrons, the energies of which are measured. The energy of the incident photons matches the ionisation energy of the sample so emitted electrons have zero kinetic energy.
ISBN:0-19-855785-X
Spectroscopy where primary electrons interact with a sample and the electrons emitted as a result of the interaction (secondary electrons) are detected.
SES
CHMO:0000411
secondary electron spectroscopy
Spectroscopy where primary electrons interact with a sample and the electrons emitted as a result of the interaction (secondary electrons) are detected.
https://orcid.org/0000-0002-0640-0422
Spectroscopy where primary electrons interact with a sample and the electrons emitted as a result of the interaction (secondary electrons) are detected as a function of emission angle.
ARSES
angle-resolved secondary electron spectrometry
angular resolved secondary electron spectrometry
angular resolved secondary electron spectroscopy
CHMO:0000412
angle-resolved secondary electron spectroscopy
Spectroscopy where primary electrons interact with a sample and the electrons emitted as a result of the interaction (secondary electrons) are detected as a function of emission angle.
https://orcid.org/0000-0002-0640-0422
Spectroscopy where primary electrons interact with a sample and the electrons emitted as a result of the interaction (secondary electrons) are detected. A magnet is used to align all electron spins parallel to the surface of the sample.
polarised secondary electron spectrometry
polarized secondary electron spectrometry
polarized secondary electron spectroscopy
spin-polarised secondary electron spectrometry
spin-polarised secondary electron spectroscopy
spin-polarized secondary electron spectrometry
spin-polarized secondary electron spectroscopy
spin-resolved secondary electron spectrometry
spin-resolved secondary electron spectroscopy
CHMO:0000413
spin-polarised secondary electron spectroscopy
Spectroscopy where primary electrons interact with a sample and the electrons emitted as a result of the interaction (secondary electrons) are detected. A magnet is used to align all electron spins parallel to the surface of the sample.
https://doi.org/10.1016/0039-6028(83)90701-X
Spectroscopy where the energies of gamma-rays emitted or absorbed by a sample is measured.
FIX:0000049
gamma ray spectrometry
gamma spectrometry
gamma spectroscopy
gamma-ray emission spectroscopy
gamma-ray spectrometry
gamma-ray spectroscopy
CHMO:0000414
gamma-ray spectroscopy
Spectroscopy where the energies of gamma-rays emitted or absorbed by a sample is measured.
https://orcid.org/0000-0002-0640-0422
A type of gamma-ray emission spectroscopy where the gamma-rays are produced by bombarding the sample with a focused beam of ions.
PIGE
PIGE spectrometry
PIGE spectroscopy
particle induced gamma-ray emission spectroscopy
particle-induced gamma-ray emission spectrometry
particle-induced prompt-photon spectrometry
particle-induced prompt-photon spectroscopy
CHMO:0000415
particle-induced gamma-ray emission spectroscopy
A type of gamma-ray emission spectroscopy where the gamma-rays are produced by bombarding the sample with a focused beam of ions.
https://orcid.org/0000-0002-0640-0422
Spectroscopy where gamma-rays are absorbed by a sample resulting in the ejection of an electron and the emission of light which is detected.
gamma-ray scattering spectrometry
CHMO:0000416
gamma-ray scattering spectroscopy
Spectroscopy where gamma-rays are absorbed by a sample resulting in the ejection of an electron and the emission of light which is detected.
https://orcid.org/0000-0002-0640-0422
Spectroscopy where the intensity of a gamma-rays beam transmitted through a solid sample is detected.
FIX:0000050
Moessbauer spectroscopy
Mossbauer spectroscopy
Mössbauer spectroscopy
Mößbauer spectroscopy
recoil-free gamma-ray resonance absorption spectroscopy
CHMO:0000417
Mossbauer spectroscopy
Spectroscopy where the intensity of a gamma-rays beam transmitted through a solid sample is detected.
https://orcid.org/0000-0002-0640-0422
Spectroscopy where gamma-rays are absorbed by a sample resulting in the ejection of conversion electrons, the energy distribution of which is measured.
DC EMS
DCEMS
DS EMS
DS MS
DSEMS
DSMS
depth-selective Mossbauer spectrometry
depth-selective Moßbauer spectrometry
depth-selective Moßbauer spectroscopy
depth-selective Mössbauer spectrometry
depth-selective Mößbauer spectrometry
depth-selective Mößbauer spectroscopy
depth-selective conversion electron Mossbauer spectrometry
depth-selective conversion electron Moßbauer spectrometry
depth-selective conversion electron Moßbauer spectroscopy
depth-selective conversion electron Mössbauer spectrometry
depth-selective conversion electron Mössbauer spectroscopy
depth-selective conversion electron Mößbauer spectrometry
depth-selective conversion electron Mößbauer spectroscopy
depth-selective electron Mossbauer spectrometry
depth-selective electron Mossbauer spectroscopy
depth-selective electron Moßbauer spectrometry
depth-selective electron Moßbauer spectroscopy
depth-selective electron Mössbauer spectrometry
depth-selective electron Mössbauer spectroscopy
depth-selective electron Mößbauer spectrometry
depth-selective electron Mößbauer spectroscopy
CHMO:0000418
depth-selective Mossbauer spectroscopy
Spectroscopy where gamma-rays are absorbed by a sample resulting in the ejection of conversion electrons, the energy distribution of which is measured.
https://orcid.org/0000-0002-0640-0422
A type of gamma-ray emission spectroscopy where atomic nuclei are excited (by a heavy ion beam or by collision with another nucleus) and their decaying gamma-ray emissions are measured.
nuclear spectrometry
CHMO:0000419
nuclear spectroscopy
A type of gamma-ray emission spectroscopy where atomic nuclei are excited (by a heavy ion beam or by collision with another nucleus) and their decaying gamma-ray emissions are measured.
https://orcid.org/0000-0002-0640-0422
A type of activation analysis where atomic nuclei are excited (by a heavy ion beam or by collision with another nucleus) and their decaying gamma-ray emissions are measured and compared to reference spectra.
NAA
CHMO:0000420
nuclear activation analysis
A type of activation analysis where atomic nuclei are excited (by a heavy ion beam or by collision with another nucleus) and their decaying gamma-ray emissions are measured and compared to reference spectra.
https://orcid.org/0000-0002-0640-0422
Spectroscopy where the change in impedance (the resistance of alternating current) of a sample during excitation is measured as a function of frequency.
dielectric spectroscopy
impedance spectrometry
IS
CHMO:0000421
impedance spectroscopy
Spectroscopy where the change in impedance (the resistance of alternating current) of a sample during excitation is measured as a function of frequency.
https://orcid.org/0000-0002-0640-0422
Spectroscopy where the change in impedance (the resistance of alternating current) of a sample during excitation with an alternating-current voltage is measured.
AC-IS
AC-impedance spectrometry
AC-impedance spectroscopy
ACIS
Ac-impedance spectrometry
Ac-impedance spectroscopy
ac-impedance spectroscopy
CHMO:0000422
alternating current impedance spectroscopy
Spectroscopy where the change in impedance (the resistance of alternating current) of a sample during excitation with an alternating-current voltage is measured.
https://orcid.org/0000-0002-0640-0422
Spectroscopy where the change in impedance (the resistance of alternating current) of an electrochemical cell is measured.
electrical impedance spectrometry
electrical-impedance spectrometry
electrical-impedance spectroscopy
electrochemical impedance spectroscopy
electrochemical-induced impedance spectrometry
EIS
CHMO:0000423
electrochemical-induced impedance spectroscopy
Spectroscopy where the change in impedance (the resistance of alternating current) of an electrochemical cell is measured.
https://orcid.org/0000-0002-0640-0422
Spectroscopy where the change in impedance (the resistance of alternating current) of a sample during laser excitation is measured.
impedance laser spectroscopy
laser induced impedance spectrometry
laser induced impedance spectroscopy
laser-induced impedance spectrometry
CHMO:0000424
laser-induced impedance spectroscopy
Spectroscopy where the change in impedance (the resistance of alternating current) of a sample during laser excitation is measured.
https://orcid.org/0000-0002-0640-0422
Spectroscopy where the absorption of emission of ions is detected.
ion spectrometry
CHMO:0000425
ion spectroscopy
Spectroscopy where the absorption of emission of ions is detected.
https://orcid.org/0000-0002-0640-0422
Spectroscopy where a focused beam of ions is directed at a sample and the secondary ions emitted are detected.
IBS
ion-beam spectrometry
CHMO:0000426
ion-beam spectroscopy
Spectroscopy where a focused beam of ions is directed at a sample and the secondary ions emitted are detected.
https://orcid.org/0000-0002-0640-0422
Spectroscopy where a focused beam of ions is directed at a sample causes binary collisions with surface molecules which result in molecular decomposition and the emission of atoms.
DRS
direct recoil spectroscopy
CHMO:0000427
direct recoil spectroscopy
Spectroscopy where a focused beam of ions is directed at a sample causes binary collisions with surface molecules which result in molecular decomposition and the emission of atoms.
https://orcid.org/0000-0002-0640-0422
Spectrocsopy where a finely focused (<10 m diameter) beam of ions is directed at a sample and the secondary ions emitted are detected.
ion micro-probe spectrometry
ion microprobe spectrometry
ion microprobe spectroscopy
CHMO:0000428
ion microprobe spectroscopy
Spectrocsopy where a finely focused (<10 m diameter) beam of ions is directed at a sample and the secondary ions emitted are detected.
https://orcid.org/0000-0002-0640-0422
Spectroscopy where a focused beam of proton is directed at a uranium sample and the secondary ions emitted are detected.
LeRIBS
low-energy radioactive ion beam spectrometry
low-energy radioactive ion beam spectroscopy
low-energy radioactive ion-beam spectrometry
CHMO:0000429
low-energy radioactive ion-beam spectroscopy
Spectroscopy where a focused beam of proton is directed at a uranium sample and the secondary ions emitted are detected.
https://orcid.org/0000-0002-0640-0422
Spectroscopy where the velocity of gas phase ions in an electric field is measured.
ion mobility spectrometry
ion-mobility spectrometry
IMS
CHMO:0000430
ion mobility spectroscopy
Spectroscopy where the velocity of gas phase ions in an electric field is measured.
ISBN:0849322472
IMS
Spectroscopy where the velocity of gas phase ions in an electric field is measured. A radio frequency voltage forces the ions to oscillate between two electrodes causing some ions to be transmitted while others collide with the walls of the electrodes.
FAIMS
high field asymmetric waveform ion mobility spectrometry
high field asymmetric waveform ion mobility spectroscopy
high-field asymmetric waveform ion mobility spectrometry
high-field asymmetric waveform ion mobility spectroscopy
DMS
CHMO:0000431
differential mobility spectroscopy
Spectroscopy where the velocity of gas phase ions in an electric field is measured. A radio frequency voltage forces the ions to oscillate between two electrodes causing some ions to be transmitted while others collide with the walls of the electrodes.
https://orcid.org/0000-0002-0640-0422
Spectroscopy where the velocity of gas phase ions in an electric field is measured. The ions are gated into a region of constant electric field strength and the ions with highest mobility arrive at the detector first.
DTIMS
drift tube ion mobility spectrometry
CHMO:0000432
drift tube ion mobility spectroscopy
Spectroscopy where the velocity of gas phase ions in an electric field is measured. The ions are gated into a region of constant electric field strength and the ions with highest mobility arrive at the detector first.
https://orcid.org/0000-0002-0640-0422
A method for determining structure where the sample is bombarded with ions (100–1000 eV) and the energies and positions of the scattered ions are detected.
ISS
ion scattering spectrometry
ion scattering spectroscopy
CHMO:0000433
ion scattering
A method for determining structure where the sample is bombarded with ions (100–1000 eV) and the energies and positions of the scattered ions are detected.
ISBN:3527296344
Spectroscopy where the sample is bombarded with He+ or H+ ions (500–1500 eV) and the energies and positions of any backscattered ions are detected.
HE IS
HE ISS
HE-IS
HE-ISS
HEIS
HEISS
RBS
Rutherford backscattering spectrometry
Rutherford scattering spectrometry
Rutherford scattering spectroscopy
backscattering spectroscopy
heavy ion scattering spectrometry
heavy ion scattering spectroscopy
heavy-ion scattering spectrometry
heavy-ion scattering spectroscopy
high-energy ion scattering spectrometry
high-energy ion scattering spectroscopy
CHMO:0000434
Rutherford backscattering spectroscopy
Spectroscopy where the sample is bombarded with He+ or H+ ions (500–1500 eV) and the energies and positions of any backscattered ions are detected.
ISBN:3527296344
Spectroscopy where the sample is illuminated with one or more laser beams and the absorption or emission of light by the sample is measured.
laser spectrometry
CHMO:0000435
laser spectroscopy
Spectroscopy where the sample is illuminated with one or more laser beams and the absorption or emission of light by the sample is measured.
https://orcid.org/0000-0002-0640-0422
Spectroscopy where the sample is illuminated with one or more laser beams and the absorption of light by the sample is measured.
LAS
laser absorbance spectrometry
laser absorbance spectroscopy
laser absorption spectrometry
CHMO:0000436
laser absorption spectroscopy
Spectroscopy where the sample is illuminated with one or more laser beams and the absorption of light by the sample is measured.
https://orcid.org/0000-0002-0640-0422
Spectroscopy where the sample is illuminated with one or more laser beams and light absorption is measured.
DLAS
direct laser absorption spectrometry
direct laser absorption spectroscopy
CHMO:0000437
direct laser absorption spectroscopy
Spectroscopy where the sample is illuminated with one or more laser beams and light absorption is measured.
https://orcid.org/0000-0002-0640-0422
Any type of laser spectroscopy where the sample is in the form of an accelerated beam of particles (atoms or ions) which is superimposed on a resonant laser beam (a laser beam with a wavelength that corresponds to an atomic transition in the sample) and light absorption is measured.
CHMO:0000438
collinear laser spectroscopy
Any type of laser spectroscopy where the sample is in the form of an accelerated beam of particles (atoms or ions) which is superimposed on a resonant laser beam (a laser beam with a wavelength that corresponds to an atomic transition in the sample) and light absorption is measured.
https://orcid.org/0000-0002-0640-0422
A type of laser spectroscopy where the sample is in the form of a high-speed accelerated beam of atoms which is superimposed on a resonant laser beam (a laser beam with a wavelength that corresponds to an atomic transition in the sample) and light absorption is measured.
CLABS
collinear fast atom beam spectrometry
collinear fast atom beam spectroscopy
CHMO:0000439
collinear fast atom-beam spectroscopy
A type of laser spectroscopy where the sample is in the form of a high-speed accelerated beam of atoms which is superimposed on a resonant laser beam (a laser beam with a wavelength that corresponds to an atomic transition in the sample) and light absorption is measured.
https://doi.org/10.1007/BF02394872
A type of laser spectroscopy where the sample is in the form of an accelerated beam of ions which is superimposed on a resonant laser beam (a laser beam with a wavelength that corresponds to an atomic transition in the sample) and light absorption is measured.
CLIBS
collinear laser beam spectrometry
collinear laser beam spectroscopy
collinear laser ion beam spectroscopy
collinear laser ion-beam spectrometry
collinear laser ion-beam spectroscopy
CHMO:0000440
collinear laser ion-beam spectroscopy
A type of laser spectroscopy where the sample is in the form of an accelerated beam of ions which is superimposed on a resonant laser beam (a laser beam with a wavelength that corresponds to an atomic transition in the sample) and light absorption is measured.
https://orcid.org/0000-0002-0640-0422
A type of laser spectroscopy where the sample is in the form of a high-speed accelerated beam of ions which is superimposed on a resonant laser beam (a laser beam with a wavelength that corresponds to an atomic transition in the sample) and light absorption is measured.
CFIBLS
collinear fast ion beam laser spectrometry
CHMO:0000441
collinear fast ion-beam laser spectroscopy
A type of laser spectroscopy where the sample is in the form of a high-speed accelerated beam of ions which is superimposed on a resonant laser beam (a laser beam with a wavelength that corresponds to an atomic transition in the sample) and light absorption is measured.
https://orcid.org/0000-0002-0640-0422
A type of laser spectroscopy where a diode laser is tuned to a specific absorption line of interest in the sample and the intensity of the transmitted radiation is measured.
TDLAS
tunable diode laser absorbance spectrometry
tunable diode laser absorbance spectroscopy
tunable diode laser absorption spectrometry
CHMO:0000442
tunable diode laser absorption spectroscopy
A type of laser spectroscopy where a diode laser is tuned to a specific absorption line of interest in the sample and the intensity of the transmitted radiation is measured.
https://orcid.org/0000-0002-0640-0422
A type of laser spectroscopy where a fixed-wavelength infrared or ultraviolet laser is used to excite the sample which is placed in an electric field. By varying the strength of the applied electric field some vibrational–rotational transitions can be made to coincide with the laser wavelength and the absorption of the laser light is measured.
Stark spectroscopy
laser Stark spectrometry
laser Stark spectroscopy
laser electric resonance spectrometry
CHMO:0000443
laser electric resonance spectroscopy
A type of laser spectroscopy where a fixed-wavelength infrared or ultraviolet laser is used to excite the sample which is placed in an electric field. By varying the strength of the applied electric field some vibrational–rotational transitions can be made to coincide with the laser wavelength and the absorption of the laser light is measured.
FIX:0000074
ISBN:0-471-96523-5
Spectroscopy where the sample is illuminated with a laser which is tuned to match an absorption frequency of the molecules in the sample.
FMS
frequency modulation spectrometry
CHMO:0000444
frequency modulation spectroscopy
Spectroscopy where the sample is illuminated with a laser which is tuned to match an absorption frequency of the molecules in the sample.
https://orcid.org/0000-0002-0640-0422
Any type of laser spectroscopy where an effect induced by the absorption of laser light is detected.
ILAS
CHMO:0000445
indirect laser absorption spectroscopy
Any type of laser spectroscopy where an effect induced by the absorption of laser light is detected.
https://orcid.org/0000-0002-0640-0422
Any type of laser spectroscopy where the sample is placed inside the laser cavity and an effect induced by the absorption of laser light is detected.
ICAS
ICL spectrometry
ICL spectroscopy
ICLAS
ICLS
intra cavity laser absorption spectroscopy
intra-cavity laser absorption spectrometry
intra-cavity laser spectrometry
intra-cavity laser spectroscopy
intracavity laser absorption spectrometry
intracavity laser absorption spectroscopy
intracavity laser spectroscopy
intracavity spectrometry
ILS
CHMO:0000446
intracavity laser absorption spectroscopy
Any type of laser spectroscopy where the sample is placed inside the laser cavity and an effect induced by the absorption of laser light is detected.
https://orcid.org/0000-0002-0640-0422
A type of laser spectroscopy where the sample is placed inside a highly reflective laser cavity and an effect induced by the absorption of laser light is detected. The laser light is tuned to match the frequency of the cavity bandwidth.
CEAS
cavity enhanced absorption spectrometry
CHMO:0000447
cavity enhanced absorption spectroscopy
A type of laser spectroscopy where the sample is placed inside a highly reflective laser cavity and an effect induced by the absorption of laser light is detected. The laser light is tuned to match the frequency of the cavity bandwidth.
https://doi.org/10.1039/b811793d
A type of laser spectroscopy where the sample is placed inside a v-shaped optical cavity and an effect induced by the absorption of laser light is detected. The laser light is allowed to feed back to the laser diode.
OF-CEAS
optical feedback cavity enhanced absorption spectrometry
CHMO:0000448
optical feedback cavity enhanced absorption spectroscopy
A type of laser spectroscopy where the sample is placed inside a v-shaped optical cavity and an effect induced by the absorption of laser light is detected. The laser light is allowed to feed back to the laser diode.
https://doi.org/10.1039/b811793d
A type of laser spectroscopy where the sample is placed inside a highly reflective laser cavity and an effect induced by the absorption of a supercontinuum light source is detected. The light source is tuned to match the frequency of the cavity bandwidth.
SC-CEAS
super continuum cavity enhanced absorption spectrometry
CHMO:0000449
super continuum cavity enhanced absorption spectroscopy
A type of laser spectroscopy where the sample is placed inside a highly reflective laser cavity and an effect induced by the absorption of a supercontinuum light source is detected. The light source is tuned to match the frequency of the cavity bandwidth.
https://orcid.org/0000-0002-0640-0422
A type of laser spectroscopy where the sample is placed inside a highly reflective laser cavity and an effect induced by the absorption of laser light is detected. The decay time for light exiting the cavity is determined as a function of pulsed laser wavelength.
CRDS
CRLAS
cavity ring-down laser absorption spectrometry cavity ringdown spectroscopy
cavity ring-down laser absorption spectroscopy
cavity ring-down spectrometry
cavity ringdown spectrometry
CHMO:0000450
cavity ring-down spectroscopy
A type of laser spectroscopy where the sample is placed inside a highly reflective laser cavity and an effect induced by the absorption of laser light is detected. The decay time for light exiting the cavity is determined as a function of pulsed laser wavelength.
ISBN:0-534-98144-5
Spectroscopy where a pump laser is used to excite a chromophore and the transmitted power of a probe laser is used to determine the state concentration (excited vs. non-excited) of the sample.
COMAS
CHMO:0000451
concentration modulated absorption spectroscopy
Spectroscopy where a pump laser is used to excite a chromophore and the transmitted power of a probe laser is used to determine the state concentration (excited vs. non-excited) of the sample.
https://orcid.org/0000-0002-0640-0422
Spectroscopy where the sample is illuminated with a laser and molecules in the sample dissociate following the absorption of one or more high-energy photons.
laser dissociation spectrometry
laser photo-fragmentation spectrometry
laser photo-fragmentation spectroscopy
laser photodissociation spectrometry
laser photodissociation spectroscopy
laser photofragmentation spectrometry
laser photofragmentation spectroscopy
laser-induced fragmentation spectrometry
laser-induced fragmentation spectroscopy
CHMO:0000452
laser dissociation spectroscopy
Spectroscopy where the sample is illuminated with a laser and molecules in the sample dissociate following the absorption of one or more high-energy photons.
https://doi.org/10.1016/S0009-2614(97)00994-9
Spectroscopy where the sample is illuminated with a laser and molecules in the sample dissociate following the absorption of two or more high-energy photons.
CHMO:0000453
multiphoton dissociation spectroscopy
Spectroscopy where the sample is illuminated with a laser and molecules in the sample dissociate following the absorption of two or more high-energy photons.
https://orcid.org/0000-0002-0640-0422
Spectroscopy where the sample is illuminated with a resonant laser (a laser which is tuned to match a transition within the sample) and molecules in the sample dissociate following the absorption of two or more high-energy photons.
REMPD spectrometry
REMPD spectroscopy
resonance enhanced multiphoton dissociation spectrometry
CHMO:0000454
resonance enhanced multiphoton dissociation spectroscopy
Spectroscopy where the sample is illuminated with a resonant laser (a laser which is tuned to match a transition within the sample) and molecules in the sample dissociate following the absorption of two or more high-energy photons.
https://orcid.org/0000-0002-0640-0422
Spectroscopy where a sample in the form of ions is illuminated with a resonant laser (a laser which is tuned to match a transition within the sample) and molecules in the sample dissociate following the absorption of one or more high-energy photons.
RID spectrometry
RID spectroscopy
resonance ion dissociation spectrometry
CHMO:0000455
resonance ion dissociation spectroscopy
Spectroscopy where a sample in the form of ions is illuminated with a resonant laser (a laser which is tuned to match a transition within the sample) and molecules in the sample dissociate following the absorption of one or more high-energy photons.
https://orcid.org/0000-0002-0640-0422
Spectroscopy where the sample is illuminated with a laser causing molecules in the sample to be electronically excited. The photons emitted as a result of the decay of the molecules back down to the ground state are measured.
LIF spectrometry
LIF spectroscopy
laser induced fluorescence spectrometry
laser-induced fluorescence spectrometry
laser-induced fluorescence spectroscopy
CHMO:0000456
laser induced fluorescence spectroscopy
Spectroscopy where the sample is illuminated with a laser causing molecules in the sample to be electronically excited. The photons emitted as a result of the decay of the molecules back down to the ground state are measured.
https://orcid.org/0000-0002-0640-0422
Spectroscopy where the energy generated by nonradiative thermal relaxation after laser light absorption is measured.
TLS
thermal lens spectrometry
CHMO:0000457
thermal lens spectroscopy
Spectroscopy where the energy generated by nonradiative thermal relaxation after laser light absorption is measured.
https://doi.org/10.1021/ac05196u
Spectroscopy where the energy generated by nonradiative thermal relaxation after visible laser light absorption is measured.
visible TLS
visible-TLS
CHMO:0000458
visible thermal lens spectroscopy
Spectroscopy where the energy generated by nonradiative thermal relaxation after visible laser light absorption is measured.
https://doi.org/10.1021/ac05196u
Spectroscopy where the energy generated by nonradiative thermal relaxation after ultraviolet laser light absorption is measured.
UV TLS
UV-TLS
ultra-violet thermal lens spectrometry
ultra-violet thermal lens spectroscopy
ultraviolet thermal lens spectrometry
ultraviolet thermal lens spectroscopy
CHMO:0000459
ultraviolet thermal lens spectroscopy
Spectroscopy where the energy generated by nonradiative thermal relaxation after ultraviolet laser light absorption is measured.
https://doi.org/10.1021/ac05196u
Spectroscopy where a thermally-excited vapour sample is illuminated with an ultraviolet or visible laser and the photon emission spectrum of the sample is observed.
laser emission spectrometry
LES
CHMO:0000460
laser emission spectroscopy
Spectroscopy where a thermally-excited vapour sample is illuminated with an ultraviolet or visible laser and the photon emission spectrum of the sample is observed.
https://orcid.org/0000-0002-0640-0422
Spectroscopy where a thermally-excited vapour sample is illuminated with a finely focused (<10 m diameter) ultraviolet or visible laser and the photon emission spectrum of the sample is observed.
LAMES
laser micro emission spectrometry
CHMO:0000461
laser micro emission spectroscopy
Spectroscopy where a thermally-excited vapour sample is illuminated with a finely focused (<10 m diameter) ultraviolet or visible laser and the photon emission spectrum of the sample is observed.
https://doi.org/10.1351/goldbook.L03473
Spectroscopy where a sample is illuminated with a laser and photoexcitation is used to promote an atom or molecule above its ionisation potential to create an ion.
laser ionisation spectrometry
laser ionization spectrometry
LIS
CHMO:0000462
laser ionisation spectroscopy
Spectroscopy where a sample is illuminated with a laser and photoexcitation is used to promote an atom or molecule above its ionisation potential to create an ion.
https://orcid.org/0000-0002-0640-0422
Spectroscopy where a sample is illuminated with resonant laser light (using a laser which is tuned to match an electronic transition within the sample) and photoexcitation is used to promote an atom or molecule above its ionisation potential to create an ion.
reonance enhanced ionization spectrometry
resonance enhanced ionisation spectrometry
resonance enhanced ionisation spectroscopy
resonance enhanced ionization spectrometry
resonance enhanced ionization spectroscopy
resonance ionisation spectrometry
resonance ionization spectrometry
resonance ionization spectroscopy
RIS
CHMO:0000463
resonance ionisation spectroscopy
Spectroscopy where a sample is illuminated with resonant laser light (using a laser which is tuned to match an electronic transition within the sample) and photoexcitation is used to promote an atom or molecule above its ionisation potential to create an ion.
https://orcid.org/0000-0002-0640-0422
Spectroscopy where resonant laser illumination (using a laser which is tuned to match an electronic transition within the sample) is used to ehanced the collisional ionisation of atoms (or molecules) occurring in a flame.
LEI spectrometry
LEI spectroscopy
LEIS
laser enhanced ionisation mass spectrometry
laser enhanced ionisation spectroscopy
laser enhanced ionization mass spectrometry
laser enhanced ionization spectroscopy
laser-enhanced ionisation spectrometry
laser-enhanced ionization spectrometry
r resonance-enhanced laser ionisation spectroscopy
r resonance-enhanced laser ionization spectroscopy
resonance-enhanced ionisation spectrometry
resonance-enhanced ionization spectrometry
CHMO:0000464
laser-enhanced ionisation spectroscopy
Spectroscopy where resonant laser illumination (using a laser which is tuned to match an electronic transition within the sample) is used to ehanced the collisional ionisation of atoms (or molecules) occurring in a flame.
https://doi.org/ja9870200573
Spectroscopy where a sample is illuminated with a laser and photoexcitation (by the absorption of two or more photons) is used to promote an atom or molecule above its ionisation potential to create an ion.
laser multiphoton ionisation spectrometry
laser multiphoton ionization spectrometry
CHMO:0000465
laser multiphoton ionisation spectroscopy
Spectroscopy where a sample is illuminated with a laser and photoexcitation (by the absorption of two or more photons) is used to promote an atom or molecule above its ionisation potential to create an ion.
https://orcid.org/0000-0002-0640-0422
Spectroscopy where a sample is illuminated with resonant laser light (using a laser which is tuned to match an electronic transitions within the sample) and photoexcitation (by the absorption of two or more photons) is used to promote an atom or molecule above its ionisation potential to create an ion.
REMPI
REMPI spectrometry
REMPI spectroscopy
resonance enhanced multiphoton ionisation spectrometry
resonance enhanced multiphoton ionization spectrometry
resonance-enhanced multiphoton ionisation spectrometry
resonance-enhanced multiphoton ionisation spectroscopy
resonance-enhanced multiphoton ionization spectrometry
resonance-enhanced multiphoton ionization spectroscopy
CHMO:0000466
resonance enhanced multiphoton ionisation spectroscopy
Spectroscopy where a sample is illuminated with resonant laser light (using a laser which is tuned to match an electronic transitions within the sample) and photoexcitation (by the absorption of two or more photons) is used to promote an atom or molecule above its ionisation potential to create an ion.
https://doi.org/10.1039/b814133a
Spectroscopy where the sample is illuminated with one or more finely focused (<10 m diameter) laser beams and the absorption or emission of light by the sample is measured.
laser micro-probe spectrometry
laser microanalysis
laser microprobe spectrometry
laser microprobe spectroscopy
CHMO:0000467
laser microprobe spectroscopy
Spectroscopy where the sample is illuminated with one or more finely focused (<10 m diameter) laser beams and the absorption or emission of light by the sample is measured.
https://orcid.org/0000-0002-0640-0422
Spectroscopy where the sample is illuminated with one or more finely focused (<10 m diameter) resonant laser beams (lasers which have been tuned to match an electronic transition within the sample) and the absorption or emission of light by the sample is measured.
resonance enhanced laser microanalysis
resonance-enchanced laser micro-probe spectrometry
resonance-enhanced laser microprobe spectrometry
resonance-enhanced laser microprobe spectroscopy
CHMO:0000468
resonance-enhanced laser microprobe spectroscopy
Spectroscopy where the sample is illuminated with one or more finely focused (<10 m diameter) resonant laser beams (lasers which have been tuned to match an electronic transition within the sample) and the absorption or emission of light by the sample is measured.
https://orcid.org/0000-0002-0640-0422
Spectroscopy where the current passing through a gas discharge is monitored as a laser light source is tuned through the frequencies of allowed transitions for excited atoms in the discharge.
optogalvanic spectrometry
CHMO:0000469
optogalvanic spectroscopy
Spectroscopy where the current passing through a gas discharge is monitored as a laser light source is tuned through the frequencies of allowed transitions for excited atoms in the discharge.
https://orcid.org/0000-0002-0640-0422
Spectrometry where the sample is converted into gaseous ions which are characterised by their mass-to-charge ratio and relative abundance.
MS
mass spectroscopy
CHMO:0000470
mass spectrometry
Spectrometry where the sample is converted into gaseous ions which are characterised by their mass-to-charge ratio and relative abundance.
FIX:0000047
https://doi.org/10.1351/goldbook.M03746
Mass spectrometry where the sample is ionised and the ions are accelerated to very high kinetic energies.
AMS
accelerator MS
accelerator mass spectrometry
accelerator mass spectroscopy
CHMO:0000471
acceleration mass spectrometry
Mass spectrometry where the sample is ionised and the ions are accelerated to very high kinetic energies.
FIX:0000707
https://orcid.org/0000-0002-0640-0422
Mass spectrometry where the sample is ionised by interaction (electron or proton transfer) with reagent (N2, O2, H2O) gaseous ions at low pressure. Reagent ions are produced by electron ionisation.
CI-MS
LCPIMS
LP-CI-MS
LPCI-MS
chemical ionisation mass spectroscopy
chemical ionization mass spectrometry
chemical ionization mass spectroscopy
low pressure chemical ionisation mass spectrometry
low pressure chemical ionisation mass spectroscopy
low pressure chemical ionization mass spectrometry
low pressure chemical ionization mass spectroscopy
CHMO:0000472
chemical ionisation mass spectrometry
Mass spectrometry where the sample is ionised by interaction (electron or proton transfer) with reagent (N2, O2, H2O) gaseous ions at low pressure. Reagent ions are produced by electron ionisation.
FIX:0000088
https://doi.org/10.1351/goldbook.C01026
Mass spectrometry where the sample is ionised by interaction (electron or proton transfer) with reagent (N2, O2, H2O) gaseous ions at atmospheric pressure. Reagent ions are produced by electron ionisation with electrons from a radioactive beta-source or a corona discharge.
APCI MS
APCI-MS
atmospheric pressure chemical ionisation mass spectroscopy
atmospheric pressure chemical ionization mass spectrometry
atmospheric pressure chemical ionization mass spectroscopy
CHMO:0000473
atmospheric pressure chemical ionisation mass spectrometry
Mass spectrometry where the sample is ionised by interaction (electron or proton transfer) with reagent (N2, O2, H2O) gaseous ions at atmospheric pressure. Reagent ions are produced by electron ionisation with electrons from a radioactive beta-source or a corona discharge.
FIX:0000866
ISBN:978-0-470-51634-8
Mass spectrometry where the sample is dissolved in a volatile solvent and dropped onto a heated filament before being ionised by interaction (electron or proton transfer) with reagent (N2, O2, H2O) gaseous ions at low pressure. Reagent ions are produced by electron ionisation.
DCI MS
DCI-MS
desorption chemical ionisation mass spectroscopy
desorption chemical ionization mass spectroscopy
direct chemical ionisation mass spectrometry
direct chemical ionisation mass spectroscopy
direct chemical ionization mass spectrometry
direct chemical ionization mass spectroscopy
in-beam ionisation mass spectrometry
in-beam ionisation mass spectroscopy
in-beam ionization mass spectrometry
in-beam ionization mass spectroscopy
CHMO:0000474
desorption chemical ionisation mass spectrometry
Mass spectrometry where the sample is dissolved in a volatile solvent and dropped onto a heated filament before being ionised by interaction (electron or proton transfer) with reagent (N2, O2, H2O) gaseous ions at low pressure. Reagent ions are produced by electron ionisation.
ISBN:978-0-470-51634-8
Mass spectrometry where the sample is ionised by interaction with reagent gaseous anions at low pressure.
negative ion chemical ionisation mass spectroscopy
negative ion chemical ionization mass spectrometry
negative ion chemical ionization mass spectroscopy
CHMO:0000475
negative ion chemical ionisation mass spectrometry
Mass spectrometry where the sample is ionised by interaction with reagent gaseous anions at low pressure.
ISBN:0-534-98144-5
Mass spectrometry where the sample is ionised by interaction with reagent gaseous cations at low pressure.
positive ion chemical ionisation mass spectroscopy
positive ion chemical ionization mass spectrometry
positive ion chemical ionization mass spectroscopy
CHMO:0000476
positive ion chemical ionisation mass spectrometry
Mass spectrometry where the sample is ionised by interaction with reagent gaseous cations at low pressure.
ISBN:0-534-98144-5
Mass spectrometry where the sample is ionised and selected ions are allowed to collide with neutral gas molecules resulting in fragmentation.
MS-CAD
MS-CID
collision induced dissociation mass spectrometry
collision induced dissociation mass spectroscopy
collisionally activated dissociation mass spectrometry
collisionally-activated dissociation mass spectrometry
CHMO:0000477
collision-induced dissociation mass spectrometry
Mass spectrometry where the sample is ionised and selected ions are allowed to collide with neutral gas molecules resulting in fragmentation.
ISBN:978-0-470-51634-8
Mass spectrometry where the sample is ionised by interaction with thermal electrons (electrons with energy 0.1 eV or less).
ECNI
electron capture negative ionisation mass spectroscopy
electron capture negative ionization mass spectroscopy
resonant electron capture negative ionisation mass spectrometry
resonant electron capture negative ionisation mass spectroscopy
resonant electron capture negative ionization mass spectrometry
resonant electron capture negative ionization mass spectroscopy
CHMO:0000478
electron capture negative ionisation mass spectrometry
Mass spectrometry where the sample is ionised by interaction with thermal electrons (electrons with energy 0.1 eV or less).
ISBN:9780470516348
true
Mass spectrometry where the sample is ionised by electrons (energy 70 eV) which have been emitted from a glowing filament and accelerated through an electric field.
CHMO:0000479
FIX:0000089
EI-MS
electron impact mass spectrometry
electron ionisation mass spectroscopy
electron ionization mass spectrometry
electron ionization mass spectroscopy
electron impact ionisation mass spectrometry
electron-impact ionisation mass spectrosopy
electron-impact ionization mass spectrosopy
CHMO:0000480
electron ionisation mass spectrometry
Mass spectrometry where the sample is ionised by electrons (energy 70 eV) which have been emitted from a glowing filament and accelerated through an electric field.
ISBN:9780534981445
Mass spectrometry where the sample is atomised using an electrothermal (resistively-heated) furnace and then ionised by electrons (energy 70 eV) which have been emitted from a glowing filament and accelerated through an electric field.
furnace atomization electron ionization mass spectroscopy
CHMO:0000481
furnace atomisation electron ionisation mass spectrometry
Mass spectrometry where the sample is atomised using an electrothermal (resistively-heated) furnace and then ionised by electrons (energy 70 eV) which have been emitted from a glowing filament and accelerated through an electric field.
USPat:5316955
Spectrometry where the sample is ionised by electrospray ionization. The ions are then characterised by their mass-to-charge ratio and relative abundance.
FIX:0000079
ES-MS
ESI MS
ESI-MS
ESI-mass spectrometry
ESIMS
ESMS
MS (EI)
electrospray ionisation mass spectroscopy
electrospray ionization mass spectrometry
electrospray ionization mass spectroscopy
electrospray mass spectrometry
CHMO:0000482
electrospray ionisation mass spectrometry
Spectrometry where the sample is ionised by electrospray ionization. The ions are then characterised by their mass-to-charge ratio and relative abundance.
ISBN:9780470516348
Electrospray ionisation mass spectrometry where the sample is ionised by forcing a solution (usually in an organic solvent) of the sample through a small cold (10-80 C) capillary (at a flow rate of 1-10 L min1).
CSI-MS
cold-spray ionisation mass spectroscopy
cold-spray ionization mass spectrometry
cold-spray ionization mass spectroscopy
CHMO:0000483
cold-spray ionisation mass spectrometry
Electrospray ionisation mass spectrometry where the sample is ionised by forcing a solution (usually in an organic solvent) of the sample through a small cold (10-80 C) capillary (at a flow rate of 1-10 L min1).
https://orcid.org/0000-0002-0640-0422
Mass spectrometry where the sample is ionised by directing charged solvent droplets (which are formed by forcing the solvent through a small heated capillary into an electric field) at the sample surface. The droplets form a thin film on the sample surface, dissolving the analyte of interest.
DESI MS
DESI-MS
DESIMS
desorption electrospray ionisation mass spectroscopy
desorption electrospray ionization mass spectroscopy
CHMO:0000484
desorption electrospray ionisation mass spectrometry
Mass spectrometry where the sample is ionised by directing charged solvent droplets (which are formed by forcing the solvent through a small heated capillary into an electric field) at the sample surface. The droplets form a thin film on the sample surface, dissolving the analyte of interest.
ISBN:978-0-470-51634-8
Mass spectrometry where the sample is ionised by forcing a solution (usually in an organic solvent) of the sample through a small heated capillary (at a flow rate of 1–10 L min-1) into an electric field to produce a very fine mist of charged droplets. When the ions are analysed using their mass-to-charge ratios the exact mass is determined as opposed to the nominal mass (the number of protons and neutrons).
HR ESI-MS
HR-ESI-MS
HRESIMS
high resolution electrospray ionisation mass spectrometry
high resolution electrospray ionisation mass spectroscopy
high resolution electrospray ionization mass spectroscopy
CHMO:0000485
high-resolution electrospray ionisation mass spectrometry
Mass spectrometry where the sample is ionised by forcing a solution (usually in an organic solvent) of the sample through a small heated capillary (at a flow rate of 1–10 L min-1) into an electric field to produce a very fine mist of charged droplets. When the ions are analysed using their mass-to-charge ratios the exact mass is determined as opposed to the nominal mass (the number of protons and neutrons).
https://orcid.org/0000-0002-0640-0422
Mass spectrometry where the sample is ionised by forcing an aqueous solution of the sample through a small heated capillary (at a flow rate of 1-10 L min1) into an electric field to produce a very fine mist of charged droplets.
FIX:0000862
ISI-MS
ISI/MS
ISMS
ion spray ionisation mass spectrometry
ion spray ionization mass spectrometry
ionspray MS
ionspray mass spectroscopy
pneumatically-assisted electrospray ionisation mass spectrometry
pneumatically-assisted electrospray ionisation mass spectroscopy
pneumatically-assisted electrospray ionization mass spectrometry
pneumatically-assisted electrospray ionization mass spectroscopy
turbo ion-spray mass spectrometry
turbo ion-spray mass spectroscopy
CHMO:0000486
ionspray mass spectrometry
Mass spectrometry where the sample is ionised by forcing an aqueous solution of the sample through a small heated capillary (at a flow rate of 1-10 L min1) into an electric field to produce a very fine mist of charged droplets.
https://orcid.org/0000-0002-0640-0422
Mass spectrometry where the sample is ionised by forcing a solution (usually in an organic solvent) of the sample through a small heated capillary (at a flow rate of 1 L min-1) into an electric field to produce a very fine mist of charged droplets.
micro-ESI-MS
microESI-MS
microelectrospray ionisation mass spectroscopy
microelectrospray ionization mass spectroscopy
CHMO:0000487
microelectrospray ionisation mass spectrometry
Mass spectrometry where the sample is ionised by forcing a solution (usually in an organic solvent) of the sample through a small heated capillary (at a flow rate of 1 L min-1) into an electric field to produce a very fine mist of charged droplets.
ISBN:0824740823
Mass spectrometry where the sample is ionised by forcing a solution (usually in an organic solvent) of the sample through a small heated capillary (at a flow rate of nL min-1) into an electric field to produce a very fine mist of charged droplets.
nano-ESI-MS
nano-electrospray mass spectrometry
nanoESI-MS
nanoelectrospray ionisation mass spectroscopy
nanoelectrospray ionization mass spectrometry
nanoelectrospray ionization mass spectroscopy
CHMO:0000488
nanoelectrospray ionisation mass spectrometry
Mass spectrometry where the sample is ionised by forcing a solution (usually in an organic solvent) of the sample through a small heated capillary (at a flow rate of nL min-1) into an electric field to produce a very fine mist of charged droplets.
ISBN:0824740823
A method where the sample mixture is first separated by high-performance liquid chromatography before being ionised by forcing a solution (usually in an organic solvent) of the sample through a small heated capillary (at a flow rate of nL min1) into an electric field to produce a very fine mist of charged droplets. The ions are then characterised by their mass-to-charge ratio and relative abundance.
HPLC-nano-HPLC
HPLC-nanoESI
high performance liquid chromatography-nanoelectrospray ionisation mass spectroscopy
high performance liquid chromatography-nanoelectrospray ionization mass spectrometry
high performance liquid chromatography-nanoelectrospray ionization mass spectroscopy
CHMO:0000489
high-performance liquid chromatography-nanoelectrospray ionisation mass spectrometry
A method where the sample mixture is first separated by high-performance liquid chromatography before being ionised by forcing a solution (usually in an organic solvent) of the sample through a small heated capillary (at a flow rate of nL min1) into an electric field to produce a very fine mist of charged droplets. The ions are then characterised by their mass-to-charge ratio and relative abundance.
ISBN:0824740823
Mass spectrometry where the sample ionised by spraying it with a very fine mist of charged droplets which was produced by forcing a solvent through a small heated capillary (at a flow rate of 1–10 L min-1) into an electric field.
SESI
secondary electrospray ionisation mass spectroscopy
secondary electrospray ionization mass spectroscopy
CHMO:0000490
secondary electrospray ionisation mass spectrometry
Mass spectrometry where the sample ionised by spraying it with a very fine mist of charged droplets which was produced by forcing a solvent through a small heated capillary (at a flow rate of 1–10 L min-1) into an electric field.
ISBN:978-0-470-51634-8
Mass spectrometry where the sample is ionised by interaction with a high electric field.
FIX:0000913
FI-MS
FI/MS
FIMS
field ionisation mass spectroscopy
field ionization mass spectroscopy
CHMO:0000491
field ionisation mass spectrometry
Mass spectrometry where the sample is ionised by interaction with a high electric field.
https://doi.org/10.1351/goldbook.F02360
Mass spectrometry where the sample is deposited on a solid surface known as an 'emitter' and ionised by interaction with a high electric field.
FD mass spectrometry
FD-MS
FDMS
field desorption mass spectroscopy
CHMO:0000492
field desorption mass spectrometry
Mass spectrometry where the sample is deposited on a solid surface known as an 'emitter' and ionised by interaction with a high electric field.
FIX:0000087
https://doi.org/10.1351/goldbook.F02357
Mass spectrometry where the sample is pyrolysed then deposited on a solid surface known as an 'emitter' and ionised by interaction with a high electric field.
Py-FDMS
PyFDMS
py-FDMS
pyFDMS
pyrolysis field desorption mass spectroscopy
pyrolysis-field desorption mass spectrometry
pyrolysis-field desorption mass spectroscopy
CHMO:0000493
pyrolysis field desorption mass spectrometry
Mass spectrometry where the sample is pyrolysed then deposited on a solid surface known as an 'emitter' and ionised by interaction with a high electric field.
https://orcid.org/0000-0002-0640-0422
Mass spectrometry where the sample is ionised by interaction with a high electric field. When the ions are analysed using their mass-to-charge ratios the 'exact' mass is determined as opposed to the 'nominal' mass (the number of protons and neutrons).
HR-FIMS
HRFIMS
high resolution field ionisation mass spectroscopy
high resolution field ionization mass spectrometry
high resolution field ionization mass spectroscopy
high-resolution field ionisation mass spectrometry
high-resolution field ionisation mass spectroscopy
high-resolution field ionization mass spectrometry
high-resolution field ionization mass spectroscopy
CHMO:0000494
high resolution field ionisation mass spectrometry
Mass spectrometry where the sample is ionised by interaction with a high electric field. When the ions are analysed using their mass-to-charge ratios the 'exact' mass is determined as opposed to the 'nominal' mass (the number of protons and neutrons).
https://orcid.org/0000-0002-0640-0422
Mass spectrometry where the sample is pyrolysed then ionised by interaction with a high electric field.
Py-FIMS
PyFIMS
py-FIMS
pyFIMS
pyrolysis field ionisation mass spectroscopy
pyrolysis field ionization mass spectrometry
pyrolysis field ionization mass spectroscopy
pyrolysis-field ionisation mass spectrometry
pyrolysis-field ionisation mass spectroscopy
pyrolysis-field ionization mass spectrometry
pyrolysis-field ionization mass spectroscopy
CHMO:0000495
pyrolysis field ionisation mass spectrometry
Mass spectrometry where the sample is pyrolysed then ionised by interaction with a high electric field.
https://orcid.org/0000-0002-0640-0422
Mass spectrometry where the sample is pyrolysed then ionised by interaction with a high electric field. The ions are analysed using their mass-to-charge ratios as a function of temperature during pyrolysis.
temperature programmed pyrolysis field ionisation mass spectrometry
temperature programmed pyrolysis field ionisation mass spectroscopy
temperature programmed pyrolysis field ionization mass spectrometry
temperature programmed pyrolysis field ionization mass spectroscopy
temperature resolved pyrolysis field ionisation mass spectrometry
temperature resolved pyrolysis field ionization mass spectrometry
temperature-programmed pyrolysis field ionisation mass spectrometry
temperature-programmed pyrolysis field ionisation mass spectroscopy
temperature-programmed pyrolysis field ionization mass spectrometry
temperature-programmed pyrolysis field ionization mass spectroscopy
temperature-resolved pyrolysis field ionisation mass spectrometry
temperature-resolved pyrolysis field ionisation mass spectroscopy
temperature-resolved pyrolysis field ionization mass spectrometry
temperature-resolved pyrolysis field ionization mass spectroscopy
CHMO:0000496
temperature-resolved pyrolysis field ionisation mass spectrometry
Mass spectrometry where the sample is pyrolysed then ionised by interaction with a high electric field. The ions are analysed using their mass-to-charge ratios as a function of temperature during pyrolysis.
https://orcid.org/0000-0002-0640-0422
Any method where a sample mixture is first separated by gas chromatography then ionised and characterised according to mass-to-charge ratio and relative abundance.
FIX:0000921
GC MS
GC-MS
GC/MS
GCMS
gas chromatography mass spectrometry
gas chromatography mass spectroscopy
gas chromatography with mass spectrometric detection
gas chromatography-mass spectroscopy
gas chromatography/mass spectrometry
CHMO:0000497
gas chromatography-mass spectrometry
Any method where a sample mixture is first separated by gas chromatography then ionised and characterised according to mass-to-charge ratio and relative abundance.
https://orcid.org/0000-0002-0640-0422
Mass spectrometry where the 'exact' mass of the molecular ions in the sample is determined as opposed to the 'nominal' mass (the number of protons and neutrons).
HR-MS
HRMS
high resolution mass spectroscopy
high-resolution mass spectrometry
CHMO:0000498
high-resolution mass spectrometry
Mass spectrometry where the 'exact' mass of the molecular ions in the sample is determined as opposed to the 'nominal' mass (the number of protons and neutrons).
https://doi.org/10.1039/b815384c
Spectrometry where the ionic species associated with the peaks in an ion mobility spectrum are identified by a mass spectrometer.
IMS MS
IMS-MS
IMS/MS
IMSMS
ion mobility spectrometry mass spectrometry
ion mobility spectrometry-mass spectrometry
ion mobility spectroscopy mass spectroscopy
ion mobility spectroscopy-mass spectroscopy
CHMO:0000499
ion mobility spectrometry-mass spectrometry
Spectrometry where the ionic species associated with the peaks in an ion mobility spectrum are identified by a mass spectrometer.
https://doi.org/10.1039/b815384c
Mass spectrometry where the mass-to-charge ratio of the sample ions is measured whilst the ions are held in a stable orbit by an electric or magnetic field.
IT MS
IT-MS
ITMS
ion trap MS
ion trap mass spectroscopy
ion-trap mass spectrometry
ion-trap mass spectroscopy
CHMO:0000500
ion trap mass spectrometry
Mass spectrometry where the mass-to-charge ratio of the sample ions is measured whilst the ions are held in a stable orbit by an electric or magnetic field.
FIX:0000917
https://orcid.org/0000-0002-0640-0422
Mass spectrometry where the mass-to-charge ratio of the sample ions is determined by measuring their cyclotron frequency (the frequency at which they precesses in a fixed magnetic field).
ICR MS
ICR mass spectrometry
ICR mass spectroscopy
ICR-MS
ICRMS
ion cyclotron resonance mass spectroscopy
ion-cyclotron-resonance mass spectrometry
ion-cyclotron-resonance mass spectroscopy
CHMO:0000501
ion cyclotron resonance mass spectrometry
Mass spectrometry where the mass-to-charge ratio of the sample ions is determined by measuring their cyclotron frequency (the frequency at which they precesses in a fixed magnetic field).
https://orcid.org/0000-0002-0640-0422
Mass spectrometry where the mass-to-charge ratio of the sample ions is determined by measuring their cyclotron frequency (the frequency at which they precesses in a fixed magnetic field) and subjecting it to a Fourier transform.
FT ICR MS
FT-ICR MS
FT-ICR mass spectrometry
FT-ICR mass spectroscopy
FT-ICR-MS
FT-ICRMS
FT/ICR mass spectrometry
FT/ICR mass spectroscopy
FTICRMS
FTMS
Fourier transform ion cyclotron resonance mass spectroscopy
Fourier transform mass spectrometry
Fourier transform mass spectroscopy
ICR-FT-MS
in-beam Fourier-transform ion cyclotron resonance
ion cyclotron resonance Fourier transform mass spectrometry
CHMO:0000502
Fourier transform ion cyclotron resonance mass spectrometry
Mass spectrometry where the mass-to-charge ratio of the sample ions is determined by measuring their cyclotron frequency (the frequency at which they precesses in a fixed magnetic field) and subjecting it to a Fourier transform.
FIX:0000083
https://doi.org/10.1351/goldbook.F02492
Mass spectrometry where the mass-to-charge ratio of the sample ions is determined by measuring their cyclotron frequency (the frequency at which they precesses in a fixed magnetic field). The 'exact' mass of the sample ions is determined as opposed to the 'nominal' mass (the number of protons and neutrons).
HR FT/ICR MS
HR-FT-ICR MS
HR-FT-ICR-MS
HR-FT-ICRMS
HR-FTICRMS
high resolution Fourier transform ion cyclotron resonance mass spectrometry
high resolution Fourier transform ion cyclotron resonance mass spectroscopy
CHMO:0000503
high-resolution Fourier transform ion cyclotron resonance mass spectrometry
Mass spectrometry where the mass-to-charge ratio of the sample ions is determined by measuring their cyclotron frequency (the frequency at which they precesses in a fixed magnetic field). The 'exact' mass of the sample ions is determined as opposed to the 'nominal' mass (the number of protons and neutrons).
https://orcid.org/0000-0002-0640-0422
Mass spectrometry where the mass-to-charge ratio of the sample ions is measured whilst the ions are held in a stable orbit by an electric field generated by four parallel electrodes.
QMS
quadrapole mass spectrometry
quadrupolar mass spectrometry
quadrupolar mass spectroscopy
quadrupole MS
quadrupole ion trap mass spectrometry
quadrupole ion trap mass spectroscopy
quadrupole ion-trap mass spectrometry
quadrupole ion-trap mass spectroscopy
quadrupole mass spectroscopy
CHMO:0000504
quadrupole mass spectrometry
Mass spectrometry where the mass-to-charge ratio of the sample ions is measured whilst the ions are held in a stable orbit by an electric field generated by four parallel electrodes.
FIX:0000094
FIX:0000095
https://doi.org/10.1016/0168-1176(90)85042-Z
Mass spectrometry where the mass-to-charge ratio of the sample ions is measured whilst the ions are held in a stable orbit by an electric field generated by three electrodes.
3D Q-MS
3D QMS
3D quadrupole MS
3D-Q-MS
3D-QMS
three-dimensional quadrupole mass spectroscopy
CHMO:0000505
three-dimensional quadrupole mass spectrometry
Mass spectrometry where the mass-to-charge ratio of the sample ions is measured whilst the ions are held in a stable orbit by an electric field generated by three electrodes.
https://orcid.org/0000-0002-0640-0422
Mass spectrometry where the relative abundance of isotopes in a sample is determined.
IR MS
IR-MS
IRMS
isotope ratio mass spectroscopy
isotope-ratio mass spectrometry
isotopic ratios mass spectrometry
isotopic ratios mass spectroscopy
CHMO:0000506
isotope ratio mass spectrometry
Mass spectrometry where the relative abundance of isotopes in a sample is determined.
https://orcid.org/0000-0002-0640-0422
Mass spectrometry where the sample is first subject to elemental analysis (dropped onto a heated reactor which contains an oxidant–-such as copper and chromium oxide–-and combusted at 900 C to produce N2, NOx, H2O and CO2 which are reduced in a stream of helium) before the relative abundance of isotopes in the sample is determined.
EA-IR-MS
EA-IRMS
elemental analyser isotope ratio mass spectrometry
elemental analyser isotope ratio mass spectroscopy
elemental analysis isotope ratio mass spectroscopy
CHMO:0000507
elemental analysis isotope ratio mass spectrometry
Mass spectrometry where the sample is first subject to elemental analysis (dropped onto a heated reactor which contains an oxidant–-such as copper and chromium oxide–-and combusted at 900 C to produce N2, NOx, H2O and CO2 which are reduced in a stream of helium) before the relative abundance of isotopes in the sample is determined.
https://doi.org/10.1039/b808232d
A method where a sample mixture is first separated by gas chromatography before being characterised according to mass-to-charge ratio and relative abundance of isotopes.
GC IRMS
GC-IR-MS
GC-IRMS
gas chromatography isotope ratio mass spectrometry
gas chromatography isotope ratio mass spectroscopy
CHMO:0000508
gas chromatography-isotope ratio mass spectrometry
A method where a sample mixture is first separated by gas chromatography before being characterised according to mass-to-charge ratio and relative abundance of isotopes.
https://doi.org/10.1039/b808232d
A method where a sample mixture is first separated by liquid chromatography before it is ionised and the relative abundance of isotopes in the sample is determined.
LC IR MS
LC-IR-MS
LC-IRMS
liquid chromatography isotope ratio mass spectrometry
liquid chromatography isotope ratio mass spectroscopy
CHMO:0000509
liquid chromatography-isotope ratio mass spectrometry
A method where a sample mixture is first separated by liquid chromatography before it is ionised and the relative abundance of isotopes in the sample is determined.
https://doi.org/10.1039/b808232d
Mass spectrometry where the relative abundance of isotopes in a sample is determined by using an isotope dilution standard (the sample labelled with a rare isotope).
ID-MS
IDMS
isotope dilution mass spectroscopy
CHMO:0000510
isotope dilution mass spectrometry
Mass spectrometry where the relative abundance of isotopes in a sample is determined by using an isotope dilution standard (the sample labelled with a rare isotope).
https://doi.org/10.1039/b614612k
Mass spectrometry where the sample is ionised by a plasma which has been generated by electromagnetic induction. The relative abundance of isotopes in the sample is then determined by using an isotope dilution standard (the sample labelled with a rare isotope).
ID-ICP-MS
ID-ICPMS
isotope dilution-inductively coupled plasma mass spectroscopy
CHMO:0000511
isotope dilution inductively coupled plasma mass spectrometry
Mass spectrometry where the sample is ionised by a plasma which has been generated by electromagnetic induction. The relative abundance of isotopes in the sample is then determined by using an isotope dilution standard (the sample labelled with a rare isotope).
https://orcid.org/0000-0002-0640-0422
A method where a sample mixture is first separated by high-performance liquid chromatography before being ionised by a plasma which has been generated by electromagnetic induction. The ions are then characterised according to mass-to-charge ratio and the relative abundance of isotopes in the sample is determined using an isotope dilution standard (the sample labelled with a rare isotope).
HPLC-ID-ICP-MS
HPLC-ID-ICPMS
high performance liquid chromatography isotope dilution inductively coupled plasma mass spectrometry
high performance liquid chromatography isotope dilution inductively coupled plasma mass spectroscopy
CHMO:0000512
high-performance liquid chromatography-isotope dilution inductively coupled plasma mass spectrometry
A method where a sample mixture is first separated by high-performance liquid chromatography before being ionised by a plasma which has been generated by electromagnetic induction. The ions are then characterised according to mass-to-charge ratio and the relative abundance of isotopes in the sample is determined using an isotope dilution standard (the sample labelled with a rare isotope).
https://orcid.org/0000-0002-0640-0422
Mass spectrometry where the sample is ionised by a plasma which has been generated by electromagnetic induction. The mass-to-charge ratios of the ions in the sample are then measured whilst the ions are held in a stable orbit by an electric field generated by four parallel electrodes. The relative abundance of isotopes in the sample is determined by using an isotope dilution standard (the sample labelled with a rare isotope).
ID-ICP-Q-MS
ID-ICP-QMS
isotope dilution inductively coupled plasma quadrupole mass spectroscopy
CHMO:0000513
isotope dilution inductively coupled plasma quadrupole mass spectrometry
Mass spectrometry where the sample is ionised by a plasma which has been generated by electromagnetic induction. The mass-to-charge ratios of the ions in the sample are then measured whilst the ions are held in a stable orbit by an electric field generated by four parallel electrodes. The relative abundance of isotopes in the sample is determined by using an isotope dilution standard (the sample labelled with a rare isotope).
https://orcid.org/0000-0002-0640-0422
Mass spectrometry where the relative abundance of non-radioactive isotopes in a sample is determined.
S-IRMS
SIRMS
stable isotope ratio mass spectroscopy
CHMO:0000514
stable isotope ratio mass spectrometry
Mass spectrometry where the relative abundance of non-radioactive isotopes in a sample is determined.
https://orcid.org/0000-0002-0640-0422
Mass spectrometry where the sample is vaporised and ionised using a high-energy pulsed laser.
FIX:0000080
LDI MS
LDI mass spectrometry
LDI-MS
LDIMS
LDMS
LIMA
LIMS
laser desorption mass spectrometry
laser desorption mass spectroscopy
laser desorption-ionisation mass spectrometry
laser desorption-ionisation mass spectroscopy
laser desorption-ionization mass spectroscopy
laser ionisation MS
laser ionisation mass analysis
laser ionisation mass spectrometry
laser ionisation mass spectroscopy
laser ionization MS
laser ionization mass analysis
laser ionization mass spectrometry
laser ionization mass spectroscopy
laser-ionisation mass analysis
laser-ionization mass analysis
CHMO:0000515
laser desorption-ionisation mass spectrometry
Mass spectrometry where the sample is vaporised and ionised using a high-energy pulsed laser.
https://orcid.org/0000-0002-0640-0422
Mass spectrometry where the sample is vaporised and ionised using a finely focused (<10 um diameter) high-energy pulsed laser.
LAMMA
LAMMS
LMMS
laser micro mass spectrometry
laser micro-probe mass analysis
laser micro-probe mass spectrometry
laser microprobe mass spectrometry
laser microprobe mass spectroscopy
laser-assisted mass microanalysis
CHMO:0000516
laser microprobe mass spectrometry
Mass spectrometry where the sample is vaporised and ionised using a finely focused (<10 um diameter) high-energy pulsed laser.
https://orcid.org/0000-0002-0640-0422
Mass spectrometry using negative ionisation where a high-energy pulsed laser is used for sample vaporisation.
negative ion laser desorption mass spectroscopy
negative ion laser desorption-ionisation mass spectrometry
negative ion laser desorption-ionisation mass spectroscopy
negative ion laser desorption-ionization mass spectrometry
negative ion laser desorption-ionization mass spectroscopy
CHMO:0000517
negative ion laser desorption mass spectrometry
Mass spectrometry using negative ionisation where a high-energy pulsed laser is used for sample vaporisation.
https://orcid.org/0000-0002-0640-0422
Mass spectrometry using positive ionisation where a high-energy pulsed laser is used for sample vaporisation.
positive ion laser desorption mass spectroscopy
positive ion laser desorption-ionisation mass spectrometry
positive ion laser desorption-ionisation mass spectroscopy
positive ion laser desorption-ionization mass spectrometry
positive ion laser desorption-ionization mass spectroscopy
CHMO:0000518
positive ion laser desorption mass spectrometry
Mass spectrometry using positive ionisation where a high-energy pulsed laser is used for sample vaporisation.
https://orcid.org/0000-0002-0640-0422
Mass spectrometry where the sample (usually a large organic molecule or biomolecule) is vaporised and ionised using a high-energy pulsed laser. The sample is held in a matrix (such as crystallised dihydrobenzoic acid) to protect it from direct laser illumination and to separate the sample molecules.
FIX:0000001
MALDI MS
MALDI-MS
MALDIMS
matrix-assisted laser desorption ionization (MALDI) MS
matrix-assisted laser desorption-ionisation mass spectroscopy
matrix-assisted laser desorption-ionization mass spectroscopy
CHMO:0000519
matrix-assisted laser desorption-ionisation mass spectrometry
Mass spectrometry where the sample (usually a large organic molecule or biomolecule) is vaporised and ionised using a high-energy pulsed laser. The sample is held in a matrix (such as crystallised dihydrobenzoic acid) to protect it from direct laser illumination and to separate the sample molecules.
ISBN:978-0-470-51634-8
Matrix-assisted laser desorption-ionisation mass spectrometry where the sample ions are accelerated to the same (known) kinetic energy and the time taken for each ion to reach a detector at a known distance is measured. This time is dependent on the mass-to-charge ratio of the ion.
FIX:0000920
MADI-TOF MS
MALDI-TOF MS
MALDI-TOF-MS
MALDI-TOF/MS
matrix assisted laser desorption ionisation time of flight mass spectrometry
matrix assisted laser desorption ionisation time of flight mass spectroscopy
matrix assisted laser desorption ionisation time-of-flight mass spectrometry
matrix assisted laser desorption ionization time of flight mass spectrometry
matrix assisted laser desorption ionization time of flight mass spectroscopy
matrix assisted laser desorption/ionisation time of flight mass spectrometry
matrix assisted laser desorption/ionisation time of flight mass spectroscopy
matrix assisted laser desorption/ionization time of flight mass spectrometry
matrix assisted laser desorption/ionization time of flight mass spectroscopy
matrix-assisted laser desorption ionization (MALDI-TOF) mass spectrometry (MS)
matrix-assisted laser desorption-ionisation time-of-flight mass spectrometry
matrix-associated laser desorption/ionization-time of flight mass spectrometry
CHMO:0000520
matrix-assisted laser desorption-ionisation time-of-flight mass spectrometry
Matrix-assisted laser desorption-ionisation mass spectrometry where the sample ions are accelerated to the same (known) kinetic energy and the time taken for each ion to reach a detector at a known distance is measured. This time is dependent on the mass-to-charge ratio of the ion.
https://orcid.org/0000-0002-0640-0422
Mass spectrometry where the sample (usually a large organic molecule or biomolecule) is vaporised and ionised using a high-energy pulsed laser. The sample is held in a sol-gel matrix to protect it from direct laser illumination and to separate the sample molecules.
SGALDI MS
SGALDI-MS
sol-gel-assisted laser desorption-ionisation mass spectrometry
sol-gel-assisted laser desorption-ionisation mass spectroscopy
sol-gel-assisted laser desorption-ionization mass spectroscopy
CHMO:0000521
sol-gel-assisted laser desorption-ionisation mass spectrometry
Mass spectrometry where the sample (usually a large organic molecule or biomolecule) is vaporised and ionised using a high-energy pulsed laser. The sample is held in a sol-gel matrix to protect it from direct laser illumination and to separate the sample molecules.
https://orcid.org/0000-0002-0640-0422
Mass spectrometry where the sample (usually a large organic molecule or biomolecule) is vaporised and ionised using a high-energy pulsed laser. The sample is mixed with a matrix compound (such as crystallised dihydrobenzoic acid) and deposited on a surface, with some chemical functionality, to protect it from direct laser illumination and to separate the sample molecules.
SALDI MS
SELDI MS
SELDI-MS
surface-assisted laser desorption-ionisation mass spectrometry
surface-assisted laser desorption-ionisation mass spectroscopy
surface-assisted laser desorption-ionization mass spectrometry
surface-assisted laser desorption-ionization mass spectroscopy
surface-enhanced laser desorption-ionisation mass spectrometry
surface-enhanced laser desorption-ionisation mass spectroscopy
surface-enhanced laser desorption-ionization mass spectrometry
surface-enhanced laser desorption-ionization mass spectroscopy
CHMO:0000522
surface-enhanced laser desorption-ionisation mass spectrometry
Mass spectrometry where the sample (usually a large organic molecule or biomolecule) is vaporised and ionised using a high-energy pulsed laser. The sample is mixed with a matrix compound (such as crystallised dihydrobenzoic acid) and deposited on a surface, with some chemical functionality, to protect it from direct laser illumination and to separate the sample molecules.
https://orcid.org/0000-0002-0640-0422
A method where a sample mixture is first separated by liquid chromatography before being vaporised and ionised using a high-energy pulsed laser, and characterised by mass-to-charge ratio and relative abundance. The sample (usually a large organic molecule or biomolecule) is held in a matrix (such as dihydrobenzoic acid) to protect it from direct laser illumination and to separate the sample molecules.
LC-MALDI-MS
liquid chromatography matrix-assisted laser desorption-ionisation mass spectrometry
liquid chromatography matrix-assisted laser desorption-ionisation mass spectroscopy
liquid chromatography matrix-assisted laser desorption-ionization mass spectroscopy
CHMO:0000523
liquid chromatography-matrix-assisted laser desorption-ionisation mass spectrometry
A method where a sample mixture is first separated by liquid chromatography before being vaporised and ionised using a high-energy pulsed laser, and characterised by mass-to-charge ratio and relative abundance. The sample (usually a large organic molecule or biomolecule) is held in a matrix (such as dihydrobenzoic acid) to protect it from direct laser illumination and to separate the sample molecules.
https://doi.org/10.1039/b812533c
A method where a sample mixture is first separated by liquid chromatography before being converted into ions which are characterised by their mass-to-charge ratio and relative abundance.
FIX:0000924
LC MS
LC-MS
LC/MS
LCMS
iquid chromatography/mass spectrometry
liquid chromatography mass spectrometry
CHMO:0000524
liquid chromatography-mass spectrometry
A method where a sample mixture is first separated by liquid chromatography before being converted into ions which are characterised by their mass-to-charge ratio and relative abundance.
https://orcid.org/0000-0002-0640-0422
Mass spectrometry where the sample is irradiated with an ultraviolet laser. The sample absorbs one or more photons resulting in ionisation.
FIX:0000906
PI-MS
PI/MS
PIMS
photoionisation mass spectroscopy
photoionization mass spectroscopy
CHMO:0000525
photoionisation mass spectrometry
Mass spectrometry where the sample is irradiated with an ultraviolet laser. The sample absorbs one or more photons resulting in ionisation.
https://orcid.org/0000-0002-0640-0422
Mass spectrometry where the sample is irradiated with an ultraviolet laser at atmospheric pressure. The sample absorbs one or more photons resulting in ionisation.
FIX:0000907
APPI MS
APPI-MS
APPIMS
atmospheric pressure photoionisation mass spectroscopy
atmospheric pressure photoionization mass spectrometry
atmospheric pressure photoionization mass spectroscopy
CHMO:0000526
atmospheric pressure photoionisation mass spectrometry
Mass spectrometry where the sample is irradiated with an ultraviolet laser at atmospheric pressure. The sample absorbs one or more photons resulting in ionisation.
https://orcid.org/0000-0002-0640-0422
Mass spectrometry where the sample is irradiated with an ultraviolet laser. The sample absorbs two or more photons resulting in ionisation.
MPI-MS
MPIMS
multi photon ionisation mass spectroscopy
multi photon ionization mass spectroscopy
multiphoton ionisation mass spectrometry
multiphoton ionisation mass spectroscopy
multiphoton ionization mass spectrometry
multiphoton ionization mass spectroscopy
μPI-MS
CHMO:0000527
multiphoton ionisation mass spectrometry
Mass spectrometry where the sample is irradiated with an ultraviolet laser. The sample absorbs two or more photons resulting in ionisation.
https://doi.org/10.1002/anie.198804473
Mass spectrometry where the sample is irradiated with a resonant laser (a laser beam with a wavelength that corresponds to an atomic transition in the sample). The sample absorbs one or more photons resulting in ionisation.
REMPI MS
resonance-enhanced mass spectrometry
CHMO:0000528
resonance-enhanced multiphoton ionisation mass spectrometry
Mass spectrometry where the sample is irradiated with a resonant laser (a laser beam with a wavelength that corresponds to an atomic transition in the sample). The sample absorbs one or more photons resulting in ionisation.
https://orcid.org/0000-0002-0640-0422
Mass spectrometry where the sample is irradiated with a resonant laser (a laser beam with a wavelength that corresponds to an atomic transition in the sample). The sample absorbs two or more photons resulting in ionisation.
RIMS
resonance ionisation mass spectroscopy
resonance ionization mass spectrometry
resonance ionization mass spectroscopy
resonance-ionization mass spectrometry
resonance-ionization mass spectroscopy
CHMO:0000529
resonance ionisation mass spectrometry
Mass spectrometry where the sample is irradiated with a resonant laser (a laser beam with a wavelength that corresponds to an atomic transition in the sample). The sample absorbs two or more photons resulting in ionisation.
https://orcid.org/0000-0002-0640-0422
Mass spectrometry where ionisation is achieved using a pneumatic nebuliser which turns the sample solution into a supersonic spray of small droplets. Ions are formed when the solvent evaporates and the statistically unbalanced charge distribution on the droplets leads to a net charge.
SSI-MS
SSI/MS
SSIMS
sonic spray ionisation mass spectrometry
sonic spray ionization mass spectrometry
sonic spray mass spectroscopy
CHMO:0000530
sonic spray mass spectrometry
Mass spectrometry where ionisation is achieved using a pneumatic nebuliser which turns the sample solution into a supersonic spray of small droplets. Ions are formed when the solvent evaporates and the statistically unbalanced charge distribution on the droplets leads to a net charge.
https://orcid.org/0000-0002-0640-0422
Mass spectrometry where a pressurised solution of the sample is forced through a heated metal capillary tip. Ions are formed when the solvent evaporates and the statistically unbalanced charge distribution on the droplets leads to a net charge.
TMS
TSP MS
TSP-MS
thermospray mass spectroscopy
CHMO:0000531
thermospray mass spectrometry
Mass spectrometry where a pressurised solution of the sample is forced through a heated metal capillary tip. Ions are formed when the solvent evaporates and the statistically unbalanced charge distribution on the droplets leads to a net charge.
https://orcid.org/0000-0002-0640-0422
Mass spectrometry where ionisation is achieved by loading the sample onto a heated filament.
TIMS
suface ionisation mass spetroscopy
suface ionization mass spetroscopy
surface ionisation mass spectrometry
surface ionization mass spectrometry
surface ionization mass spectroscopy
thermal ionisation mass spectroscopy
thermal ionization mass spectroscopy
thermal-ionization mass spectrometry
thermal-ionization mass spectroscopy
CHMO:0000532
thermal ionisation mass spectrometry
Mass spectrometry where ionisation is achieved by loading the sample onto a heated filament.
FIX:0000912
ISBN:0-534-98144-5
Mass spectrometry where a liquid sample passes through a desolvation chamber producing a beam of microscopic solid particles.
PB MS
PB-MS
particle beam mass spectroscopy
particle-beam mass spectrometry
particle-beam mass spectroscopy
CHMO:0000533
particle beam mass spectrometry
Mass spectrometry where a liquid sample passes through a desolvation chamber producing a beam of microscopic solid particles.
https://orcid.org/0000-0002-0640-0422
Mass spectrometry where the sample is ionised in a plasma (a partially ionised gas, such as Ar, containing free electrons).
plasma source mass spectroscopy
PS-MS
CHMO:0000534
plasma mass spectrometry
Mass spectrometry where the sample is ionised in a plasma (a partially ionised gas, such as Ar, containing free electrons).
https://orcid.org/0000-0002-0640-0422
Plasma mass spectrometry where the plasma has been generated by a potential difference between two electrodes, one of which is grounded and one of which is live.
CCP MS
capacitively coupled plasma mass spectroscopy
CHMO:0000535
capacitively coupled plasma mass spectrometry
Plasma mass spectrometry where the plasma has been generated by a potential difference between two electrodes, one of which is grounded and one of which is live.
https://orcid.org/0000-0002-0640-0422
Plasma mass spectrometry where the plasma has been generated by superimposing a static magnetic field and a high-frequency electromagnetic field at the electron cyclotron resonance frequency (the frequency at which an electron precesses in a magnetic field).
ECR-MS
ECR/MS
electron cyclotron resonance mass spectroscopy
CHMO:0000536
electron cyclotron resonance mass spectrometry
Plasma mass spectrometry where the plasma has been generated by superimposing a static magnetic field and a high-frequency electromagnetic field at the electron cyclotron resonance frequency (the frequency at which an electron precesses in a magnetic field).
https://orcid.org/0000-0002-0640-0422
Plasma mass spectrometry where the plasma has been generated by passing an electrical discharge between two electrodes under reduced pressure. The ions are then characterised by their mass-to-charge ratio and relative abundance.
GD-MS
GD/MS
glow discharge ionisation mass spectrometry
glow discharge ionisation mass spectroscopy
glow discharge ionization mass spectrometry
glow discharge ionization mass spectroscopy
glow-discharge mass spectroscopy
CHMO:0000537
glow-discharge mass spectrometry
Plasma mass spectrometry where the plasma has been generated by passing an electrical discharge between two electrodes under reduced pressure. The ions are then characterised by their mass-to-charge ratio and relative abundance.
https://orcid.org/0000-0002-0640-0422
Plasma mass spectrometry where the plasma has been generated by electromagnetic induction.
FIX:0000863
ICP-MS
ICPMS
inductively coupled plasma-mass spectrometry
inductively coupled plasma-mass spectroscopy
CHMO:0000538
inductively coupled plasma mass spectrometry
Plasma mass spectrometry where the plasma has been generated by electromagnetic induction.
https://orcid.org/0000-0002-0640-0422
Plasma mass spectrometry where the sample is vaporised by depositing it on a probe which is rapidly heated (to >1000 deg C) by passing a current through it.
FIX:0000864
ETV-ICP-MS
ETV-ICPMS
electrothermal vaporisation inductively coupled plasma mass spectroscopy
electrothermal vaporization inductively coupled plasma mass spectrometry
electrothermal vaporization inductively coupled plasma mass spectroscopy
CHMO:0000539
electrothermal vaporisation inductively coupled plasma mass spectrometry
Plasma mass spectrometry where the sample is vaporised by depositing it on a probe which is rapidly heated (to >1000 deg C) by passing a current through it.
ISBN:978-0-470-51634-8
ETV-ICP-MS where the solid sample is prepared by grinding into a fine powder and suspension in a diluent such as 0.1% HNO3.
slurry electrothermal vaporisation inductively coupled plasma mass spectroscopy
slurry electrothermal vaporization inductively coupled plasma mass spectrometry
slurry electrothermal vaporization inductively coupled plasma mass spectroscopy
slurry sampling electrothermal vaporisation inductively coupled plasma mass spectrometry
slurry sampling electrothermal vaporisation inductively coupled plasma mass spectroscopy
slurry sampling electrothermal vaporization inductively coupled plasma mass spectrometry
slurry sampling electrothermal vaporization inductively coupled plasma mass spectroscopy
CHMO:0000540
slurry electrothermal vaporisation inductively coupled plasma mass spectrometry
ETV-ICP-MS where the solid sample is prepared by grinding into a fine powder and suspension in a diluent such as 0.1% HNO3.
ISBN:1566701554
Mass spectrometry where a solid sample is ground to a fine powder and suspended in a diluent (such as 0.1% HNO3) before being vaporised by a probe which is rapidly heated by passing a current through it. The vaporised sample is ionised in a plasma (a partially ionised gas–-such as Ar–-containing free electrons) which has been generated by electromagnetic induction.
SN-ETV-ICP-MS
SN-ETV-ICPMS
slurry nebulisation electrothermal vaporisation inductively coupled plasma mass spectroscopy
slurry nebulization electrothermal vaporization inductively coupled plasma mass spectrometry
slurry nebulization electrothermal vaporization inductively coupled plasma mass spectroscopy
CHMO:0000541
slurry nebulisation electrothermal vaporisation inductively coupled plasma mass spectrometry
Mass spectrometry where a solid sample is ground to a fine powder and suspended in a diluent (such as 0.1% HNO3) before being vaporised by a probe which is rapidly heated by passing a current through it. The vaporised sample is ionised in a plasma (a partially ionised gas–-such as Ar–-containing free electrons) which has been generated by electromagnetic induction.
https://orcid.org/0000-0002-0640-0422
Mass spectrometry where a solid sample is vaporised by depositing it on a probe which is rapidly heated by passing a current through it. The vaporised sample is ionised in a plasma (a partially ionised gas–-such as Ar–-containing free electrons) which has been generated by electromagnetic induction.
SS-ETV-ICP-MS
SS-ETV-ICPMS
direct solid sampling electrothermal vaporisation inductively coupled plasma mass spectroscopy
direct solid sampling electrothermal vaporization inductively coupled plasma mass spectrometry
direct solid sampling electrothermal vaporization inductively coupled plasma mass spectroscopy
direct solid-sampling electrothermal vaporisation inductively coupled plasma mass spectrometry
direct solid-sampling electrothermal vaporisation inductively coupled plasma mass spectroscopy
direct solid-sampling electrothermal vaporization inductively coupled plasma mass spectrometry
direct solid-sampling electrothermal vaporization inductively coupled plasma mass spectroscopy
solid sampling electrothermal vaporisation inductively coupled plasma mass spectroscopy
solid sampling electrothermal vaporization inductively coupled plasma mass spectrometry
solid sampling electrothermal vaporization inductively coupled plasma mass spectroscopy
solid-sampling electrothermal vaporisation inductively coupled plasma mass spectrometry
solid-sampling electrothermal vaporisation inductively coupled plasma mass spectroscopy
solid-sampling electrothermal vaporization inductively coupled plasma mass spectrometry
solid-sampling electrothermal vaporization inductively coupled plasma mass spectroscopy
CHMO:0000542
solid sampling electrothermal vaporisation inductively coupled plasma mass spectrometry
Mass spectrometry where a solid sample is vaporised by depositing it on a probe which is rapidly heated by passing a current through it. The vaporised sample is ionised in a plasma (a partially ionised gas–-such as Ar–-containing free electrons) which has been generated by electromagnetic induction.
https://orcid.org/0000-0002-0640-0422
A method where a sample mixture is first separated by high-performance liquid chromatography before being ionised in a plasma (a partially ionised gas–-such as Ar–-containing free electrons) which has been generated by electromagnetic induction, and characterised by mass-to-charge ratio and relative abundance.
HPLC ICP MS
HPLC-ICP-MS
HPLC-ICPMS
HPLC/ICP-MS
high performance liquid chromatography inductively coupled plasma mass spectrometry
high performance liquid chromatography-ICPMS
high performance liquid chromatography-inductively coupled plasma mass spectrometry
high pressure liquid chromatography inductively coupled mass spectroscopy
CHMO:0000543
high performance liquid chromatography-inductively coupled plasma mass spectrometry
A method where a sample mixture is first separated by high-performance liquid chromatography before being ionised in a plasma (a partially ionised gas–-such as Ar–-containing free electrons) which has been generated by electromagnetic induction, and characterised by mass-to-charge ratio and relative abundance.
https://doi.org/10.1039/b813118j
A method where a sample mixture is first separated by high-performance liquid chromatography with fluorescence detection before being ionised in a plasma (a partially ionised gas–-such as Ar–-containing free electrons) which has been generated by electromagnetic induction, and characterised according to mass-to-charge ratio and relative abundance.
HPLC-FD-ICP-MS
high performance liquid chromatography fluorescence detection inductively coupled plasma mass spectrometry
high performance liquid chromatography fluorescence detection inductively coupled plasma mass spectroscopy
CHMO:0000544
high-performance liquid chromatography fluorescence detection-inductively coupled plasma mass spectrometry
A method where a sample mixture is first separated by high-performance liquid chromatography with fluorescence detection before being ionised in a plasma (a partially ionised gas–-such as Ar–-containing free electrons) which has been generated by electromagnetic induction, and characterised according to mass-to-charge ratio and relative abundance.
https://orcid.org/0000-0002-0640-0422
A method where a sample mixture is first separated by high-performance liquid chromatography with photodiode array detection before being ionised in a plasma (a partially ionised gas–-such as Ar–-containing free electrons) which has been generated by electromagnetic induction, and characterised according to mass-to-charge ratio and relative abundance.
HPLC-PDA-ICP-MS
high performance liquid chromatography photodiode array inductively coupled plasma mass spectrometry
high performance liquid chromatography photodiode array inductively coupled plasma mass spectroscopy
CHMO:0000545
high-performance liquid chromatography photodiode array-inductively coupled plasma mass spectrometry
A method where a sample mixture is first separated by high-performance liquid chromatography with photodiode array detection before being ionised in a plasma (a partially ionised gas–-such as Ar–-containing free electrons) which has been generated by electromagnetic induction, and characterised according to mass-to-charge ratio and relative abundance.
https://orcid.org/0000-0002-0640-0422
Mass spectrometry where the sample is ionised in a plasma (a partially ionised gas–-such as Ar–-containing free electrons) which has been generated by electromagnetic induction. The 'exact' mass of the sample ions is then determined as opposed to the 'nominal' mass (the number of protons and neutrons).
HR-ICP-MS
HR-ICPMS
high resolution inductively coupled plasma mass spectrometry
high resolution inductively coupled plasma mass spectroscopy
CHMO:0000546
high-resolution inductively coupled plasma mass spectrometry
Mass spectrometry where the sample is ionised in a plasma (a partially ionised gas–-such as Ar–-containing free electrons) which has been generated by electromagnetic induction. The 'exact' mass of the sample ions is then determined as opposed to the 'nominal' mass (the number of protons and neutrons).
https://orcid.org/0000-0002-0640-0422
Mass spectrometry where the sample is ionised in a plasma (a partially ionised gas–-such as Ar–-containing free electrons) which has been generated by electromagnetic induction. The beam of ions is then directed into magnetic field, the orientation of which is perpendicular to the beam. The magnetic field forces the charged particles into different circular trajectories, the radii of which depend on the strength of the magnetic field, the accelerating voltage, and the mass of the ion.
ICP-SF-MS
inductively coupled plasma field sector mass spectroscopy
CHMO:0000547
inductively coupled plasma field sector mass spectrometry
Mass spectrometry where the sample is ionised in a plasma (a partially ionised gas–-such as Ar–-containing free electrons) which has been generated by electromagnetic induction. The beam of ions is then directed into magnetic field, the orientation of which is perpendicular to the beam. The magnetic field forces the charged particles into different circular trajectories, the radii of which depend on the strength of the magnetic field, the accelerating voltage, and the mass of the ion.
https://orcid.org/0000-0002-0640-0422
Mass spectrometry where the sample is ionised in a plasma (a partially ionised gas–-such as Ar–-containing free electrons) which has been generated by electromagnetic induction. The mass-to-charge ratio of the sample ions is then measured whilst the ions are held in a stable orbit by an electric field generated by three electrodes.
ICP-three dimensional-Q-MS
ICP-three dimensional-QMS
inductively coupled plasma three dimensional quadrupole mass spectroscopy
CHMO:0000548
inductively coupled plasma three dimensional quadrupole mass spectrometry
Mass spectrometry where the sample is ionised in a plasma (a partially ionised gas–-such as Ar–-containing free electrons) which has been generated by electromagnetic induction. The mass-to-charge ratio of the sample ions is then measured whilst the ions are held in a stable orbit by an electric field generated by three electrodes.
https://orcid.org/0000-0002-0640-0422
Mass spectrometry where the sample is ionised in a plasma (a partially ionised gas–-such as Ar–-containing free electrons) which has been generated by electromagnetic induction. The sample ions with different masses are then accelerated to the same (known) kinetic energy and the time taken for each ion to reach a detector at a known distance is measured.
ICP-TOF-MS
ICP-TOFMS
ICP-ToF-MS
inductively coupled plasma time of flight mass spectrometry
inductively coupled plasma time of flight mass spectroscopy
inductively coupled plasma time-of-flight mass spectroscopy
CHMO:0000549
inductively coupled plasma time-of-flight mass spectrometry
Mass spectrometry where the sample is ionised in a plasma (a partially ionised gas–-such as Ar–-containing free electrons) which has been generated by electromagnetic induction. The sample ions with different masses are then accelerated to the same (known) kinetic energy and the time taken for each ion to reach a detector at a known distance is measured.
https://orcid.org/0000-0002-0640-0422
Mass spectrometry where the sample is vaporised using a laser pulse then ionised in a plasma (a partially ionised gas–-such as Ar–-containing free electrons) which has been generated by electromagnetic induction.
LA ICP-MS
LA-ICP-MS
LA-ICPMS
laser ablation ICP-MS
laser ablation inductively coupled plasma mass spectroscopy
laser ablation-ICPMS
CHMO:0000550
laser ablation inductively coupled plasma mass spectrometry
Mass spectrometry where the sample is vaporised using a laser pulse then ionised in a plasma (a partially ionised gas–-such as Ar–-containing free electrons) which has been generated by electromagnetic induction.
ISBN:978-0-470-51634-8
Mass spectrometry where the sample is vaporised using a laser pulse then ionised in a plasma (a partially ionised gas–-such as Ar–-containing free electrons) which has been generated by electromagnetic induction. The sample ions with different masses are then accelerated to the same (known) kinetic energy and the time taken for each ion to reach a detector at a known distance is measured.
LA-ICP-TOF-MS
LA-ICP-ToF-MS
laser ablation inductively coupled plasma time of flight mass spectrometry
laser ablation inductively coupled plasma time of flight mass spectroscopy
laser ablation inductively coupled plasma time-of-flight mass spectroscopy
CHMO:0000551
laser ablation inductively coupled plasma time-of-flight mass spectrometry
Mass spectrometry where the sample is vaporised using a laser pulse then ionised in a plasma (a partially ionised gas–-such as Ar–-containing free electrons) which has been generated by electromagnetic induction. The sample ions with different masses are then accelerated to the same (known) kinetic energy and the time taken for each ion to reach a detector at a known distance is measured.
https://orcid.org/0000-0002-0640-0422
A method where a sample mixture is first separated by liquid chromatography before being ionised in a plasma (a partially ionised gas–-such as Ar–-containing free electrons) which has been generated by electromagnetic induction, and characterised by mass-to-charge ratio and relative abundance.
LC-ICP-MS
LC-ICPMS
LC/ICP-MS
liquid chromatography inductively coupled plasma mass spectroscopy
liquid chromatography-inductively coupled plasma mass spectrometry
CHMO:0000552
liquid chromatography-inductively coupled plasma mass spectrometry
A method where a sample mixture is first separated by liquid chromatography before being ionised in a plasma (a partially ionised gas–-such as Ar–-containing free electrons) which has been generated by electromagnetic induction, and characterised by mass-to-charge ratio and relative abundance.
FIX:0000865
https://orcid.org/0000-0002-0640-0422
Mass spectrometry where the sample is ionised in a plasma (a partially ionised gas–-such as Ar–-containing free electrons) which has been generated by electromagnetic induction. A series of collectors ised used to detect several ion beams simultaneously.
MC-ICP-MS
MC-ICPMS
multi collector-inductively coupled plasma mass spectrometry
multicollector inductively coupled plasma mass spectrometry
multicollector inductively coupled plasma mass spectroscopy
multiple collector inductively coupled plasma mass spectroscopy
CHMO:0000553
multiple collector inductively coupled plasma mass spectrometry
Mass spectrometry where the sample is ionised in a plasma (a partially ionised gas–-such as Ar–-containing free electrons) which has been generated by electromagnetic induction. A series of collectors ised used to detect several ion beams simultaneously.
https://doi.org/10.1039/b808232d
A method where a sample mixture is first separated by size-exclusion chromatography before being ionised in a plasma (a partially ionised gas–-such as Ar–-containing free electrons) which has been generated by electromagnetic induction, and characterised by mass-to-charge ratio and relative abundance.
CHMO:0000755
SEC-ICP-MS
SEC-ICPMS
SEC/ICPMS
size-exclusion chromatography inductively coupled mass spectrometry
size-exclusion chromatography inductively coupled mass spectroscopy
size-exclusion chromatography-inductively coupled plasma mass spectroscopy
CHMO:0000554
size-exclusion chromatography-inductively coupled plasma mass spectrometry
A method where a sample mixture is first separated by size-exclusion chromatography before being ionised in a plasma (a partially ionised gas–-such as Ar–-containing free electrons) which has been generated by electromagnetic induction, and characterised by mass-to-charge ratio and relative abundance.
https://orcid.org/0000-0002-0640-0422
A method where a sample mixture is first separated by size-exclusion and high-performance liquid chromatographies before being ionised in a plasma (a partially ionised gas–-such as Ar–-containing free electrons) which has been generated by electromagnetic induction, and characterised by mass-to-charge ratio and relative abundance.
SEC-HPLC-ICP-MS
size-exclusion chromatography-high performance liquid chromatography inductively coupled plasma mass spectrometry
size-exclusion chromatography-high performance liquid chromatography-inductively coupled plasma mass spectroscopy
CHMO:0000555
size-exclusion chromatography-high-performance liquid chromatography-inductively coupled plasma mass spectrometry
A method where a sample mixture is first separated by size-exclusion and high-performance liquid chromatographies before being ionised in a plasma (a partially ionised gas–-such as Ar–-containing free electrons) which has been generated by electromagnetic induction, and characterised by mass-to-charge ratio and relative abundance.
https://orcid.org/0000-0002-0640-0422
Mass spectrometry where a sample mixture (a solution in dilute HNO3) is ionised in a plasma (a partially ionised gas–-such as Ar–-containing free electrons) which has been generated by electromagnetic induction.
solution ICP-MS
solution ICPMS
solution inductively coupled plasma mass spectroscopy
solution-ICP-MS
CHMO:0000556
solution inductively coupled plasma mass spectrometry
Mass spectrometry where a sample mixture (a solution in dilute HNO3) is ionised in a plasma (a partially ionised gas–-such as Ar–-containing free electrons) which has been generated by electromagnetic induction.
https://orcid.org/0000-0002-0640-0422
Mass spectrometry where a sample mixture (a solution in dilute HNO3) is passed through a nebuliser to form a mist of finely dispersed droplets before being ionised in a plasma (a partially ionised gas–-such as Ar–-containing free electrons) which has been generated by electromagnetic induction.
SN-ICP-MS
solution nebulisation inductively coupled plasma mass spectroscopy
solution nebulization inductively coupled plasma mass spectrometry
solution nebulization inductively coupled plasma mass spectroscopy
CHMO:0000557
solution nebulisation inductively coupled plasma mass spectrometry
Mass spectrometry where a sample mixture (a solution in dilute HNO3) is passed through a nebuliser to form a mist of finely dispersed droplets before being ionised in a plasma (a partially ionised gas–-such as Ar–-containing free electrons) which has been generated by electromagnetic induction.
https://orcid.org/0000-0002-0640-0422
Mass spectrometry where the sample is ionised in a plasma (a partially ionised gas–-such as Ar–-containing free electrons) which has been generated by microwave radiation.
MIP MS
MIP-MS
MIPMS
microwave induced plasma mass spectrometry
microwave induced plasma mass spectroscopy
CHMO:0000558
microwave-induced plasma mass spectrometry
Mass spectrometry where the sample is ionised in a plasma (a partially ionised gas–-such as Ar–-containing free electrons) which has been generated by microwave radiation.
https://orcid.org/0000-0002-0640-0422
Mass spectrometry where the sample is ionised in a plasma (a partially ionised gas–-such as Ar–-containing free electrons) which has been generated by bombarding the sample (mounted on a thin foil) with a highly energietic fission fragment from 252Cf.
PD-MS
PD/MS
plasma desorption ionisation mass spectrometry
plasma desorption ionization mass spectrometry
plasma desorption mass spectroscopy
PDMS
CHMO:0000559
plasma desorption mass spectrometry
Mass spectrometry where the sample is ionised in a plasma (a partially ionised gas–-such as Ar–-containing free electrons) which has been generated by bombarding the sample (mounted on a thin foil) with a highly energietic fission fragment from 252Cf.
ISBN:0-534-98144-5
PDMS
Mass spectrometry where the sample is bombarded with a stream of primary mass-selected particles and the secondary ions ejected from the sample are detected.
SIMS
secondary ion mass spectroscopy
CHMO:0000560
secondary ion mass spectrometry
Mass spectrometry where the sample is bombarded with a stream of primary mass-selected particles and the secondary ions ejected from the sample are detected.
FIX:0000122
OrangeBook:17.3
Mass spectrometry where the sample is bombarded with a continuous focused beam of primary mass-selected ions which remove material from the surface of the sample by sputtering. The secondary ions ejected from the sample are then detected.
DSIMS
dynamic mass spectrometry
dynamic mass spectroscopy
dynamic secondary ion mass spectroscopy
sputtered mass spectrometry
sputtered mass spectroscopy
DMS
CHMO:0000561
dynamic secondary ion mass spectrometry
Mass spectrometry where the sample is bombarded with a continuous focused beam of primary mass-selected ions which remove material from the surface of the sample by sputtering. The secondary ions ejected from the sample are then detected.
https://orcid.org/0000-0002-0640-0422
Mass spectrometry where the sample is bombarded with a continuous focused beam of primary mass-selected ions which remove material from the surface of the sample by sputtering. The neutral atoms ejected from the sample are ionised and detected.
SNMS
dynamic neutral atom mass spectrometry
dynamic neutral atom mass spectroscopy
dynamic neutral particle mass spectrometry
dynamic neutral particle mass spectroscopy
secondary neutral atom mass spectrometry
secondary neutral atom mass spectroscopy
secondary neutral particle mass spectrometry
secondary neutral particle mass spectroscopy
sputtered neutral atom mass spectroscopy
sputtered neutral particle mass spectroscopy
CHMO:0000562
sputtered neutral atom mass spectrometry
Mass spectrometry where the sample is bombarded with a continuous focused beam of primary mass-selected ions which remove material from the surface of the sample by sputtering. The neutral atoms ejected from the sample are ionised and detected.
ISBN:3527296344
Mass spectrometry where the sample (which is held in a liquid matrix) is bombarded with a stream of primary noble gas atoms and the secondary ions ejected from the sample are detected.
FIX:0000086
FAB-MS
FABMS
LSI-MS
LSIMS
MS (FAB)
fast atom bombardment mass spectrometry
fast atom bombardment mass spectroscopy
fast-atom bombardment mass spectroscopy
liquid secondary ion mass spectrometry
liquid secondary ion mass spectroscopy
CHMO:0000563
fast-atom bombardment mass spectrometry
Mass spectrometry where the sample (which is held in a liquid matrix) is bombarded with a stream of primary noble gas atoms and the secondary ions ejected from the sample are detected.
https://doi.org/10.1351/goldbook.F02328
Mass spectrometry where the sample is bombarded with a stream of primary mass-selected particles and the secondary elemental ions (usually H+, D+ or He+) ejected from the sample are detected.
MSRI
mass spectroscopy of recoiled ions
CHMO:0000564
mass spectrometry of recoiled ions
Mass spectrometry where the sample is bombarded with a stream of primary mass-selected particles and the secondary elemental ions (usually H+, D+ or He+) ejected from the sample are detected.
https://orcid.org/0000-0002-0640-0422
Mass spectrometry where the sample is bombarded with a stream of primary mass-selected particles and the secondary ions ejected from the sample are detected by accelerating them to the same (known) kinetic energy and measuring the time taken for each ion to reach a detector at a known distance. This time is dependent on the mass-to-charge ratio of the ion.
TOF-SIMS
ToF-SIMS
time-of-flight secondary ion mass spectroscopy
CHMO:0000565
time-of-flight secondary ion mass spectrometry
Mass spectrometry where the sample is bombarded with a stream of primary mass-selected particles and the secondary ions ejected from the sample are detected by accelerating them to the same (known) kinetic energy and measuring the time taken for each ion to reach a detector at a known distance. This time is dependent on the mass-to-charge ratio of the ion.
FIX:0000959
https://orcid.org/0000-0002-0640-0422
Mass spectrometry where a surface is bombarded with sample ions and the secondary electrons emitted are detected.
SEEM-MS
SEEM/MS
secondary electron emission mass spectroscopy
CHMO:0000566
secondary electron emission mass spectrometry
Mass spectrometry where a surface is bombarded with sample ions and the secondary electrons emitted are detected.
https://doi.org/10.1016/0168-1176(89)83028-9
Spectroscopy where the energy states of 15N nuclei placed in a static magnetic field are interrogated by inducing transitions between the states via radio frequency irradiation. Each experiment consists of a sequence of radio frequency pulses with delay periods in between them.
15N NMR
15N NMR spectrometry
15N NMR spectroscopy
15N nuclear magnetic resonance spectrometry
15N-NMR
CHMO:0000567
15N nuclear magnetic resonance spectroscopy
Spectroscopy where the energy states of 15N nuclei placed in a static magnetic field are interrogated by inducing transitions between the states via radio frequency irradiation. Each experiment consists of a sequence of radio frequency pulses with delay periods in between them.
CHEBI:36934
FIX:0000136
rsc:pr
Mass spectrometry where the sample ions are directed into magnetic field, the orientation of which is perpendicular to the beam. The magnetic field forces the charged particles into different circular trajectories, the radii of which depend on the strength of the magnetic field, the accelerating voltage, and the mass of the ion.
SF-MS
SFMS
magnetic sector mass spectrometry
sector field mass spectroscopy
sector-field mass spectrometry
sector-field mass spectroscopy
CHMO:0000568
sector field mass spectrometry
Mass spectrometry where the sample ions are directed into magnetic field, the orientation of which is perpendicular to the beam. The magnetic field forces the charged particles into different circular trajectories, the radii of which depend on the strength of the magnetic field, the accelerating voltage, and the mass of the ion.
FIX:0000093
https://orcid.org/0000-0002-0640-0422
Mass spectrometry where the sample is ionised by introducing it into a tube containing fast flowing He gas and ions such as H3O+, NO+ and O2+.
SIFT-MS
selected ion flow tube mass spectroscopy
CHMO:0000569
selected ion flow tube mass spectrometry
Mass spectrometry where the sample is ionised by introducing it into a tube containing fast flowing He gas and ions such as H3O+, NO+ and O2+.
ISBN:978-0-470-51634-8
Mass spectrometry where the sample is ionised by introducing it into a tube containing fast flowing He gas and H3O+ ions.
PTR-MS
PTR/MS
PTRMS
proton transfer reaction mass spectroscopy
CHMO:0000570
proton transfer reaction mass spectrometry
Mass spectrometry where the sample is ionised by introducing it into a tube containing fast flowing He gas and H3O+ ions.
FIX:0000919
https://orcid.org/0000-0002-0640-0422
Mass spectrometry where the intensities of one or more specific ion beams are recorded rather than the entire mass spectrum.
selected ion monitoring
selected-ion monitoring
selective-ion monitoring
SIM
CHMO:0000571
selective ion monitoring
Mass spectrometry where the intensities of one or more specific ion beams are recorded rather than the entire mass spectrum.
https://doi.org/10.1351/goldbook.SO5547
SIM
Mass spectrometry where the intensity of a specific ion beam is recorded rather than the entire mass spectrum.
single ion monitoring
CHMO:0000572
single-ion monitoring
Mass spectrometry where the intensity of a specific ion beam is recorded rather than the entire mass spectrum.
https://orcid.org/0000-0002-0640-0422
Mass spectrometry where the intensities of multiple specific ion beams are recorded rather than the entire mass spectrum.
multiple ion monitoring
CHMO:0000573
multiple-ion monitoring
Mass spectrometry where the intensities of multiple specific ion beams are recorded rather than the entire mass spectrum.
https://orcid.org/0000-0002-0640-0422
Mass spectrometry where the sample is ionised by a vacuum spark discharge, which is generated by a pulsed high (25–100 kV) potential difference between two electrodes.
SSMS
spark ionisation mass spectrometry
spark ionization mass spectrometry
spark source mass spectroscopy
spark-source mass spectrometry
spark-source mass spectroscopy
CHMO:0000574
spark source mass spectrometry
Mass spectrometry where the sample is ionised by a vacuum spark discharge, which is generated by a pulsed high (25–100 kV) potential difference between two electrodes.
FIX:0000903
https://doi.org/10.1007/BF00488596
Mass spectrometry involving multiple mass-selection steps, with some form of fragmentation occurring between each stage.
MS-MS
MS/MS
MS2
double mass spectrometry
tandem MS
tandem mass spectroscopy
tandem-MS
CHMO:0000575
tandem mass spectrometry
Mass spectrometry involving multiple mass-selection steps, with some form of fragmentation occurring between each stage.
FIX:0000084
https://orcid.org/0000-0002-0640-0422
Mass spectrometry involving multiple mass-selection steps, where the sample ions are allowed to collide with neutral gas molecules (resulting in fragmentation) between each mass-selection stage.
CAD-MS/MS
CAD-MS2
CID-MS-MS
CID-MS/MS
CID-MS2
collision induced dissociation tandem mass spectrometry
collision induced dissociation tandem mass spectroscopy
collision-induced dissociation-tandem mass spectrometry
collision-induced dissociation-tandem mass spectroscopy
collisionally activated dissociation tandem mass spectrometry
CHMO:0000576
collision-induced dissociation tandem mass spectrometry
Mass spectrometry involving multiple mass-selection steps, where the sample ions are allowed to collide with neutral gas molecules (resulting in fragmentation) between each mass-selection stage.
https://orcid.org/0000-0002-0640-0422
Mass spectrometry involving multiple mass-selection steps, with some form of fragmentation occurring between each stage. Sample ionisation is achieved by forcing a solution (usually in an organic solvent) of the sample through a small heated capillary (at a flow rate of 1–10 uL min-1) into an electric field to produce a very fine mist of charged droplets.
ESI-MS/MS
ESI-MS2
electrospray ionisation tandem mass spectroscopy
electrospray ionization tandem mass spectroscopy
CHMO:0000577
electrospray ionisation tandem mass spectrometry
Mass spectrometry involving multiple mass-selection steps, with some form of fragmentation occurring between each stage. Sample ionisation is achieved by forcing a solution (usually in an organic solvent) of the sample through a small heated capillary (at a flow rate of 1–10 uL min-1) into an electric field to produce a very fine mist of charged droplets.
https://orcid.org/0000-0002-0640-0422
A method where the sample mixture is first separated by high-performance liquid chromatography before being ionised by forcing a solution (usually in an organic solvent) of it through a small heated capillary (at a flow rate of 1–10 uL min1) into an electric field to produce a very fine mist of charged droplets. The ions are then characterised according to mass-to-charge ratio and relative abundance by two mass spectrometers in series.
HPLC ESI MS-MS
HPLC ESI MS/MS
HPLC-ESI-MS-MS
HPLC-ESI-MS/MS
HPLC-ESI-MS2
high performance liquid chromatography electrospray ionisation tandem mass spectrometry
high performance liquid chromatography electrospray ionisation tandem mass spectroscopy
high pressure liquid chromatography electrospray ionisation tandem mass spectroscopy
high pressure liquid chromatography electrospray ionization tandem mass spectroscopy
CHMO:0000578
high-performance liquid chromatography-electrospray ionisation tandem mass spectrometry
A method where the sample mixture is first separated by high-performance liquid chromatography before being ionised by forcing a solution (usually in an organic solvent) of it through a small heated capillary (at a flow rate of 1–10 uL min1) into an electric field to produce a very fine mist of charged droplets. The ions are then characterised according to mass-to-charge ratio and relative abundance by two mass spectrometers in series.
https://doi.org/10.1039/b813118j
Mass spectrometry involving multiple mass-selection steps, with some form of fragmentation occurring between each stage. The mass-to-charge ratios of the sample ions are measured whilst the ions are held in a stable orbit by an electric field generated by four parallel electrodes.
TQ-MS
TQMS
tandem quadrupole mass spectroscopy
CHMO:0000579
tandem quadrupole mass spectrometry
Mass spectrometry involving multiple mass-selection steps, with some form of fragmentation occurring between each stage. The mass-to-charge ratios of the sample ions are measured whilst the ions are held in a stable orbit by an electric field generated by four parallel electrodes.
https://orcid.org/0000-0002-0640-0422
Mass spectrometry where sample ions with different masses are accelerated to the same (known) kinetic energy and the time taken for each ion to reach a detector at a known distance is measured. This time is dependent on the mass-to-charge ratio of the ion.
TOF-MS
TOFMS
ToF-MS
time-of-flight mass spectroscopy
CHMO:0000580
time-of-flight mass spectrometry
Mass spectrometry where sample ions with different masses are accelerated to the same (known) kinetic energy and the time taken for each ion to reach a detector at a known distance is measured. This time is dependent on the mass-to-charge ratio of the ion.
FIX:0000082
https://doi.org/10.1351/goldbook.T06382
Any type of chemical imaging spectroscopy where an optical microscope is used to image the sample and locate a small area for spectral analysis.
microspectrometry
CHMO:0000581
microspectroscopy
Any type of chemical imaging spectroscopy where an optical microscope is used to image the sample and locate a small area for spectral analysis.
https://orcid.org/0000-0002-0640-0422
Spectroscopy where an optical microscope is used to image the sample and locate a small area for spectral analysis with radiation in the ultraviolet to near infrared range.
MSP
CHMO:0000582
microspectrophotometry
Spectroscopy where an optical microscope is used to image the sample and locate a small area for spectral analysis with radiation in the ultraviolet to near infrared range.
https://orcid.org/0000-0002-0640-0422
true
true
Spectroscopy which probes the rotational degrees of freedom of a molecule.
FIX:0000031
CHMO:0000585
rotational spectroscopy
Spectroscopy which probes the rotational degrees of freedom of a molecule.
https://orcid.org/0000-0001-5985-7429
Spectroscopy where the sample is bombarded with radiation in the microwave region (1–1000 mm).
FIX:0000018
microwave spectrometry
CHMO:0000586
microwave spectroscopy
Spectroscopy where the sample is bombarded with radiation in the microwave region (1–1000 mm).
ISBN:048661798X
Spectroscopy where the sample is irradiated with a single pulse of radiation in the microwave region (1–1000 mm) and the spectrum is subject to a Fourier transform.
FT-MW spectrometry
FT-MW spectroscopy
FTMW spectrometry
FTMW spectroscopy
Fourier transform microwave spectrometry
CHMO:0000587
Fourier transform microwave spectroscopy
Spectroscopy where the sample is irradiated with a single pulse of radiation in the microwave region (1–1000 mm) and the spectrum is subject to a Fourier transform.
https://orcid.org/0000-0002-0640-0422
Spectroscopy where the sample (in the form of a molecular beam) is irradiated with a single pulse of radiation in the microwave region (1–1000 mm) and the spectrum is subject to a Fourier transform.
MB-FTMW spectrometry
MB-FTMW spectroscopy
molecular beam Fourier transform microwave spectrometry
CHMO:0000588
molecular beam Fourier transform microwave spectroscopy
Spectroscopy where the sample (in the form of a molecular beam) is irradiated with a single pulse of radiation in the microwave region (1–1000 mm) and the spectrum is subject to a Fourier transform.
https://doi.org/10.1039/b810940k
Spectroscopy where the sample (in the form of a molecular beam) is vaporised by laser ablation before being irradiated with a single pulse of radiation in the microwave region (1–1000 mm) and the spectrum is subject to a Fourier transform.
LA-MB-FTMW spectrometry
LA-MB-FTMW spectroscopy
laser ablation molecular beam FT microwave spectroscopy
laser ablation molecular beam Fourier transform microwave (LA-MB-FTMW) spectroscopy
laser ablation molecular beam Fourier transform microwave spectrometry
CHMO:0000589
laser ablation molecular beam Fourier transform microwave spectroscopy
Spectroscopy where the sample (in the form of a molecular beam) is vaporised by laser ablation before being irradiated with a single pulse of radiation in the microwave region (1–1000 mm) and the spectrum is subject to a Fourier transform.
https://doi.org/10.1039/b810940k
Spectroscopy where a beam of neutrons is used to probe atomic and magnetic dynamics.
inelastic neutron scattering
neutron absorption spectrometry
neutron absorption spectroscopy
neutron spectrometry
slow neutron spectrometry
slow neutron spectroscopy
CHMO:0000590
neutron spectroscopy
Spectroscopy where a beam of neutrons is used to probe atomic and magnetic dynamics.
https://orcid.org/0000-0002-0640-0422
Spectroscopy where the energy states of spin-active nuclei placed in a static magnetic field are interrogated by inducing transitions between the states via radio frequency irradiation.
FIX:0000022
NMR
NMR spectrometry
NMR spectroscopy
nuclear magnetic resonance (NMR) spectroscopy
nuclear magnetic resonance spectrometry
CHMO:0000591
NMR in practice usually refers to pulsed nuclear magnetic resonance spectrometry, CHMO:0000613
nuclear magnetic resonance spectroscopy
Spectroscopy where the energy states of spin-active nuclei placed in a static magnetic field are interrogated by inducing transitions between the states via radio frequency irradiation.
rsc:pr
Spectroscopy where the energy states of spin-active nuclei placed in a static magnetic field are interrogated by inducing transitions between the states via radio frequency irradiation. Each experiment consists of a sequence of radio frequency pulses with delay periods in between them, and the spectrum is obtained by plotting chemical shift vs. frequency.
1-D NMR
1D NMR
1D NMR spectrometry
1D NMR spectroscopy
1D nuclear magnetic resonance spectrometry
1D nuclear magnetic resonance spectroscopy
one-dimensional nuclear magnetic resonance spectrometry
one-dimensional nuclear magnetic resonance spectroscopy
CHMO:0000592
one-dimensional nuclear magnetic resonance spectroscopy
Spectroscopy where the energy states of spin-active nuclei placed in a static magnetic field are interrogated by inducing transitions between the states via radio frequency irradiation. Each experiment consists of a sequence of radio frequency pulses with delay periods in between them, and the spectrum is obtained by plotting chemical shift vs. frequency.
FIX:0000055
https://doi.org/10.1039/b808986h
Spectroscopy where the energy states of 1H nuclei placed in a static magnetic field are interrogated by inducing transitions between the states via radio frequency irradiation. Each experiment consists of a sequence of radio frequency pulses with delay periods in between them.
FIX:0000134
1H NMR
1H NMR spectroscopy
1H nuclear magnetic resonance spectrometry
1H-NMR
1H-NMR spectrometry
1H-NMR spectroscopy
proton NMR
proton nuclear magnetic resonance spectroscopy
CHMO:0000593
1H nuclear magnetic resonance spectroscopy
Spectroscopy where the energy states of 1H nuclei placed in a static magnetic field are interrogated by inducing transitions between the states via radio frequency irradiation. Each experiment consists of a sequence of radio frequency pulses with delay periods in between them.
rsc:pr
Spectroscopy where the energy states of 11B nuclei placed in a static magnetic field are interrogated by inducing transitions between the states via radio frequency irradiation. Each experiment consists of a sequence of radio frequency pulses with delay periods in between them.
11B NMR
11B NMR spectrometry
11B NMR spectroscopy
11B nuclear magnetic resonance spectrometry
11B-NMR
CHMO:0000594
11B nuclear magnetic resonance spectroscopy
Spectroscopy where the energy states of 11B nuclei placed in a static magnetic field are interrogated by inducing transitions between the states via radio frequency irradiation. Each experiment consists of a sequence of radio frequency pulses with delay periods in between them.
CHEBI:52451
FIX:0001106
rsc:pr
Spectroscopy where the energy states of 13C nuclei placed in a static magnetic field are interrogated by inducing transitions between the states via radio frequency irradiation. Each experiment consists of a sequence of radio frequency pulses with delay periods in between them.
FIX:0000135
13C NMR
13C NMR spectroscopy
13C nuclear magnetic resonance spectrometry
13C-NMR spectrometry
13C-NMR spectroscopy
C-NMR
carbon NMR
CHMO:0000595
13C nuclear magnetic resonance spectroscopy
Spectroscopy where the energy states of 13C nuclei placed in a static magnetic field are interrogated by inducing transitions between the states via radio frequency irradiation. Each experiment consists of a sequence of radio frequency pulses with delay periods in between them.
rsc:pr
Spectroscopy where the energy states of 13C nuclei placed in a static magnetic field are interrogated by inducing transitions between the states via radio frequency irradiation. Each experiment consists of a sequence of radio frequency pulses with delay periods in between them.The 13C NMR signals are enhanced by transferring 1H magnetisation to 13C nuclei and the phase of the signals reflects the multiplicity i.e. CH, CH2 or CH3). Separate methyl, methylene and methine spectra may be obtained.
DEPT
DEPT NMR
distortionless enhancement by polarisation transfer
distortionless enhancement by polarization transfer
distortionless enhancement with polarisation transfer
distortionless enhancement with polarization transfer
CHMO:0000596
distortionless enhancement with polarization transfer
Spectroscopy where the energy states of 13C nuclei placed in a static magnetic field are interrogated by inducing transitions between the states via radio frequency irradiation. Each experiment consists of a sequence of radio frequency pulses with delay periods in between them.The 13C NMR signals are enhanced by transferring 1H magnetisation to 13C nuclei and the phase of the signals reflects the multiplicity i.e. CH, CH2 or CH3). Separate methyl, methylene and methine spectra may be obtained.
FIX:0000459
rsc:pr
Spectroscopy where the energy states of 19F nuclei placed in a static magnetic field are interrogated by inducing transitions between the states via radio frequency irradiation. Each experiment consists of a sequence of radio frequency pulses with delay periods in between them.
FIX:0000137
19F NMR
19F NMR spectrometry
19F NMR spectroscopy
19F nuclear magnetic resonance spectrometry
19F-NMR
CHMO:0000597
19F nuclear magnetic resonance spectroscopy
Spectroscopy where the energy states of 19F nuclei placed in a static magnetic field are interrogated by inducing transitions between the states via radio frequency irradiation. Each experiment consists of a sequence of radio frequency pulses with delay periods in between them.
rsc:pr
An NMR experiment in which a second frequency dimension is employed to disperse the signals and reveal correlations between interacting nuclei.
2-D NMR
2D NMR
2D NMR spectrometry
2D NMR spectroscopy
2D nuclear magnetic resonance
2D nuclear magnetic resonance spectrometry
two-dimensional NMR
two-dimensional nuclear magnetic resonance spectrometry
two-dimensional nuclear magnetic resonance spectroscopy
CHMO:0000598
two-dimensional nuclear magnetic resonance spectroscopy
An NMR experiment in which a second frequency dimension is employed to disperse the signals and reveal correlations between interacting nuclei.
FIX:0000056
rsc:pr
A type of homonuclear NMR spectroscopy where a second frequency dimension is employed to disperse the signals and reveal correlations between nuclei which are J-coupled (usually <=3 bonds apart).
COSY
correlated spectrometry
correlated spectroscopy
correlation spectrometry
CHMO:0000599
correlation spectroscopy
A type of homonuclear NMR spectroscopy where a second frequency dimension is employed to disperse the signals and reveal correlations between nuclei which are J-coupled (usually <=3 bonds apart).
FIX:0000543
rsc:pr
A type of NMR spectroscopy where a second frequency dimension is employed to disperse the signals and reveal correlations between protons and heteronuclei.
FIX:0001025
2D heteronuclear correlation spectroscopy
HETCOR
HETCORR
HETCOSY
HETEROCOR
hetCOSY
heteronuclear COSY
two-dimensional heteronuclear correlation spectroscopy
CHMO:0000600
heteronuclear correlation spectroscopy
A type of NMR spectroscopy where a second frequency dimension is employed to disperse the signals and reveal correlations between protons and heteronuclei.
rsc:pr
A type of heteronuclear NMR spectroscopy where a second frequency dimension is employed to disperse the signals and reveal correlations between protons and nuclei which are 2–3 bonds removed.
FIX:0000180
HMBC
HMBC NMR
CHMO:0000601
heteronuclear multiple bond coherence
A type of heteronuclear NMR spectroscopy where a second frequency dimension is employed to disperse the signals and reveal correlations between protons and nuclei which are 2–3 bonds removed.
rsc:pr
A type of heteronuclear NMR spectroscopy where pulsed-field gradients are used and a second frequency dimension is employed to disperse the signals and reveal correlations between protons and nuclei which are 2–3 bonds removed.
GHMBC
gHMBC
gradient heteronuclear multiple bond coherence
gradient-selected HMBC
CHMO:0000602
gradient-selected heteronuclear multiple bond coherence
A type of heteronuclear NMR spectroscopy where pulsed-field gradients are used and a second frequency dimension is employed to disperse the signals and reveal correlations between protons and nuclei which are 2–3 bonds removed.
rsc:pr
A type of heteronuclear NMR spectroscopy where a second frequency dimension is employed to disperse the signals and reveal correlations between protons and the nuclei to which they are covalently bound. In HMQC the magnetisation of both nuclei is allowed to evolve over time.
FIX:0000149
HMQC
HMQC NMR
CHMO:0000603
heteronuclear multiple quantum coherence
A type of heteronuclear NMR spectroscopy where a second frequency dimension is employed to disperse the signals and reveal correlations between protons and the nuclei to which they are covalently bound. In HMQC the magnetisation of both nuclei is allowed to evolve over time.
rsc:pr
A type of heteronuclear NMR spectroscopy where a second frequency dimension is employed to disperse the signals and reveal correlations between protons and the nuclei to which they are covalently bound. In HSQC only the magnetisation of one nucleus is allowed to evolve over time.
FIX:0000148
HSQC
CHMO:0000604
heteronuclear single quantum coherence
A type of heteronuclear NMR spectroscopy where a second frequency dimension is employed to disperse the signals and reveal correlations between protons and the nuclei to which they are covalently bound. In HSQC only the magnetisation of one nucleus is allowed to evolve over time.
rsc:pr
A type of homonuclear NMR spectroscopy which reveal correlations between all nuclei of a spin-system.
FIX:0000133
FIX:0000556
HOHAHA spectrometry
HOHAHA spectroscopy